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The collective yrast band of the nucleus $^{48}$Cr is studied using thespherical shell model and the HFB method. Both approaches produce basically thesame axially symmetric intrinsic state up to the - accurately reproduced -observed backbending. Agreement between both calculations extends to mostobservables. The only significant discrepancy comes from the static moments ofinertia and can be attributed to the need of a more refined treatment ofpairing correlations in the HFB calculation.Comment: 4 pages, RevTeX 3.0 using psfig, 6 Postscript figures included using  uufile

physical review letters

Intrinsic vs Laboratory Frame Description of the Deformed Nucleus<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow /><mml:mrow><mml:mn>48</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>Cr

Intrinsic vs Laboratory Frame Description of the Deformed Nucleus48Cr