Glass experimental

M. Thommes, G. H. Findenegg, M. Schoen. Critical depletion of a pure fluid in controlled-pore glass. Experimental results and grand canonical ensemble Monte Carlo simulation. Langmuir 77 2137-2142, 1995. 

These high alkali pressures can be attributed to the presence of unreacted Na2C03 impurity in the original glass samples, even though care was taken to avoid this in the glass preparation. Residual carbonate impurity is a common problem with glass experimentation e.g., see Cable and Chaudhry (50). 

Figure 15.2 Chemiluminescence emission intensity from both the glass and the silvered surface (Ag) (Top). Insert - i tographs of the silvered and glass surfeces, with (insert - Bottom) and without (insert - Top) chemiluminescence material in tiie experimental sandwich. The enhancement factOT was > 20, i.e. intensity on Ag / intensity on glass. Experimental sample sandwich (Bottom). Reproduced frexn AppliedPf sics Letters 88 173104. (2006).

Binder K, HeermannDW (1992) Monte Carlo Simnlation in Statistical Physics. Springer-Verlag, Berlin Binder K, Young AP (1986) Spin glasses Experimental facts, theoretical concepts and open questions. Rev Mod Phys 58 801-976... 

K. Binder and A. P. Young. Spin glasses experimental facts, theoretical concepts, and open questions. Reviews of Modern Physics, 58 (1986), 801 M. Mezard, G. Parisi and M. Virasoro, Spin Glass Theory and Beyond. Singapore World Scientific (1987). 

Fig. 42. Phase diagram for LiHo,Y, F4 Ising magnet. PM, paramagne FM, ferromagnet SG, spin glass. Experimental data are from neutron scattering and magnetic susceptibility measurements (Kjaer et al. 1989, Reich et al. 1990).

Pantano, C. (1993). X-Ray Photoelectron Spectroscopy of glass experimental techniques of glass science. Westerville Ohio, American Ceramic Society. 

---