Bose-Einstein Condensation of excitons in Bilayer electron systems

the GaAs/!AlGa"As heterostructure with the parameters h=15 nm and c=60 nm. The gate potential profile !solid line" at z =h, together with the generating positive

To account for this effect the fit starts at 500 ms. The results of both measurement agree within their uncertainties.. Figure 4.3: Comparison of the three-body loss coefficient L 3

In agreement with the experimental results, the numeri- cal results also show additional structures before and after the upper turning point when a soft mirror is placed 270 mm

Die bemerkenswerte Folge davon, daß die Streul¨ange des attraktiven Wechselwirkungs- potentials V (r) zwischen den Atomen eines Kondensats auch positiv sein kann, ist die Tatsache,

In Section 6.2, we prove our main results, that is, that generalized Bose–Einstein condensation P -almost surely occurs in a wide range of intensities and contact interaction

This wave function exists only in the condensed Bose gas and takes the role of the order parameter of the phase transition to the Bose-Einstein condensate.. The order

This hope arises from two underlying concepts: the inher- ently quantum mechanical nature of spin (enabling the possibility of truly quantum devices which could not be envisioned

Tensors of the Molecular Magnetic Susceptibility and the Molecular Electric Quadrupole Moment in Pyra- zole: A High Resolution Rotational Zeeman Effect Study OG. Sutter 1248