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. 2007 Jun;36(2):277-81.
doi: 10.1016/j.neuroimage.2006.11.035. Epub 2007 Jan 16.

A BOLD search for baseline

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A BOLD search for baseline

Robert G Shulman et al. Neuroimage. 2007 Jun.

Abstract

While we occasionally observe negative BOLD signals, its physiological basis has remained uncertain. This is in part due to the qualitative use of fMRI where the baseline is conveniently differenced away to reveal focal area(s) of interest. Recently, however, there has been a noticeable trend towards quantitative neuroimaging where changes in oxidative energetics (CMR(O2)) are quantified by calibrated fMRI. Pasley et al. [Pasley, B.N., Inglis, B.A., Freeman, R.D., 2007. Analysis of oxygen metabolism implies a neural origin for the negative BOLD response in human visual cortex. NeuroImage] used calibrated fMRI in conjunction with a novel stimulus paradigm to investigate the neural basis of the negative BOLD signal in awake humans. They hypothesized - based on prior results - that if the baseline was lowered then DeltaCMR(O2) would have to be larger. While their main findings point to an energetic basis for the negative BOLD signal, their results have far reaching implications for the present definition of baseline as well as for future research investigating the neural and/or energetic basis of baseline.

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Figures

Figure 1
Figure 1
Schematic representations of possible increase (left) or decrease (right) in activity upon stimulation (black jagged arrow) from the resting, unperturbed baseline (dotted line). The modular activity, obtained by differencing, is represented by the dark rectangles and is normally used to reveal focally activated (left) or deactivated (right) regions. The remaining activity, which is represented by white rectangles, is ignored by the differencing method, which is the resting, unperturbed baseline. Modified from Shulman et al (1999).
Figure 2
Figure 2
Changes in energy consumption (CMRO2) and histogram of spiking rate (ν). Upon stimulation (black jagged arrow) from the resting, unperturbed baseline (left) the distribution of firing rates shift in congruence with the energy required for the new, perturbed state (right). Modified from Smith et al (2002).

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