<?xml version="1.0" encoding="UTF-8"?><xml><records><record><source-app name="Biblio" version="7.x">Drupal-Biblio</source-app><ref-type>17</ref-type><contributors><authors><author><style face="normal" font="default" size="100%">Pissas, M.</style></author><author><style face="normal" font="default" size="100%">Stamopoulos, D.</style></author><author><style face="normal" font="default" size="100%">Lee, S.</style></author><author><style face="normal" font="default" size="100%">Tajima, S.</style></author></authors></contributors><titles><title><style face="normal" font="default" size="100%">Vortex matter properties of carbon-substituted MgB2 single crystals</style></title><secondary-title><style face="normal" font="default" size="100%">PHYSICAL REVIEW B</style></secondary-title></titles><dates><year><style  face="normal" font="default" size="100%">2004</style></year><pub-dates><date><style  face="normal" font="default" size="100%">2004</style></date></pub-dates></dates><volume><style face="normal" font="default" size="100%">70</style></volume><isbn><style face="normal" font="default" size="100%">2469-99502469-9969</style></isbn><language><style face="normal" font="default" size="100%">eng</style></language><abstract><style face="normal" font="default" size="100%">We have studied the vortex matter phase diagram in two carbon doped MgB2-xCx (x=0.04 and 0.1) single crystals. We have found that, as in pristine MgB2, the peak effect is also present in carbon doped crystals. The regime where the peak effect is developed is more extended in comparison to the undoped crystal. The enhancement of the peak effect regime, combined with the higher H-c2(c)(0), makes doped MgB2 more favorable for practical applications. The absence of significant bulk pinning below the line H-on(T), which denotes the onset points of the peak effect, implies that the Bragg glass phase is present for H&lt;H-on(T). Interestingly the end points H-ep(T) of the peak effect are placed well below the upper critical fields H-c2(T). The unexpected absence of bulk pinning above the end-point line H-ep(T) of the peak effect implies the presence of a slightly pinned vortex phase in the regime H-ep(T)&lt;H&lt;H-c2(T).</style></abstract><issue><style face="normal" font="default" size="100%">13</style></issue></record></records></xml>