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Seamus Davis
Does a ‘hidden’ ordered electronic state exist in the underdoped ‘pseudogap’ regime of the cuprate phase diagram? This question has been the focus of intensive research worldwide. But after more than a decade of searches, no long range ordered state has been detected there. Our spectroscopic imaging STM studies of Ca2-xNaxCuO2Cl2 in that regime did reveal a 4a0X4a0 ‘checkerboard’ pattern of density-of-state modulations1 which persisted into the low doped superconducting region. But the actual charge density modulation in the ‘checkerboard’ pattern is negligible. So, to examine the doped-hole density in Ca2-xNaxCuO2Cl2 directly, we have recently developed new imaging techniques. We find atomic-scale variations in hole-density which have no long range order but, instead, look like a ‘hole glass’ with short range 4a0X4a0 correlations. Embedded in this ‘hole glass’ are more ordered nano-regions of dimensions ~4a0X16a0. It seems plausible that the ‘checkerboard’ density-of-state modulations are due to scattering of quasiparticles by the Coulomb potential of this 4a0X4a0 correlated ‘hole glass’. I will discuss the relationship of these observations to results from other probes and argue that the electronic state in lightly-doped cuprates has not been hidden, merely overlooked. I will also discuss the likelihood that this type of ‘hole glass’ is, in fact, the native state of lightly doped cuprates (when dopant disorder is present). __________________________________1Hanaguri et al., Nature 430, 1001 (2004)
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