p. 1 BORDERS OF MULTIPLE VISUAL AREAS IN HUMANS REVEALED BY FUNCTIONAL MRI
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1 p. 1 BORDERS OF MULTIPLE VISUAL AREAS IN HUMANS REVEALED BY FUNCTIONAL MRI M.I. Sereno *, A.M. Dale, J.B. Reppas, K.K. Kwong, J.W. Belliveau, T.J. Brady, B.R. Rosen, and R.B.H. Tootell M.I. Sereno, A.M. Dale, Cognitive Science 0515, University of California, San Diego, La Jolla, CA , USA. J.B. Reppas, Harvard-MIT Division of Health Sciences and Technology, Boston, MA 02115, USA. K.K. Kwong, J.W. Belliveau, T.J. Brady, B.R. Rosen, R.B.H. Tootell, MGH NMR Center, th Street, Charlestown, MA 02129, USA. * [email protected] Published as: Sereno, M.I., A.M. Dale, J.B. Reppas, K.K. Kwong, J.W. Belliveau, T.J. Brady, B.R. Rosen, and R.B.H. Tootell (1995) Borders of multiple visual areas in human revealed by functional magnetic resonance imaging. Science 268: ABSTRACT The borders of human visual areas V1, V2, VP, V3, and V4 were precisely and non-invasively determined. Functional magnetic resonance images were recorded during phase-encoded retinal stimulation. This volume data set was then sampled with a cortical surface reconstruction, making it possible to calculate local visual field sign (mirror vs. non-mirror image representation). This method automatically and objectively outlines area borders because adjacent areas often have the opposite field sign. Cortical magnification factor curves for striate and extrastriate cortical areas were determined, which showed that human visual areas have a greater emphasis on the center of gaze than their counterparts in monkeys. Retinotopically organized visual areas in humans extend anteriorly to overlap several areas previously shown to be activated by written words. Over half of the neocortex in non-human primates is occupied by visual areas. At least 25 visual areas beyond the primary visual cortex (V1) have been identified with a combination of microelectrode mapping, tracer injections, histological stains, and functional studies (1). The analysis of this data has been greatly aided by the use of flattened representations of the cortical surface made from conventional sections using graphical techniques (2) and flattened wire models (3), or more directly from sections of physically flatmounted cortex (4). A large portion of the neocortex in the human primate is likely to be occupied by visual areas too. It has been difficult, however, to outline unambiguously any human cortical area with non-invasive techniques. Previous studies mapped only a few locations in the visual field, or have relied on stimulus features to activate different areas (5); and the tortuous convolutions of the human neocortex have defied previous attempts to see activity across all of its surface area at once. Many of the cortical visual areas in non-human primates are retinotopically organized to some degree (3, 6). These areas are irregularly shaped and somewhat variable in location; consequently, recordings from many locations ( ) in single animals have been required in order to define areal borders with confidence (7). Here we demonstrate a technique for generating retinotopic maps of visual cortex in humans with a precision similar to that obtained in the most detailed invasive animal studies. Responses to phase-encoded retinal stimulation (8) were recorded with echo-planar functional magnetic resonance imaging (9) and analyzed with a Fourier-based method. The resulting volume data sets were sampled with a cortical surface reconstruction made from high resolution structural MRI images collected separately for each subject (10). The cortical surface containing the data was then unfolded and analyzed with the visual field sign method to distinguish mirror image from non-mirror image representations (7). By combining these four techniques (multislice functional MRI, stimulus phase-encoding and Fourier analysis, cortical surface reconstruction, and visual field sign calculations) it was possible to reconstruct the retinotopic organization of V1, V2, VP, V3, and V4 in humans in two dimensions, and to accurately trace out the borders between these areas in the living human brain. To map polar angle, 128 asymmetric spin echo MRI images (11) of 8-16 oblique sections perpendicular to the calcarine sulcus ( total) were obtained in a 512 sec session (~8.5 min) while subjects (n = 7) viewed a slowly rotating (clockwise or counterclockwise), semicircular checkerboard stimulus. Eccentricity was mapped using a thick ring (dilating or contracting) instead of a semicircle. These four kinds of stimuli elicit periodic excitation at the rotation or dilation/contraction frequency at each point in a cortical retinotopic map (8, 12). The phase of the periodic response at the rotation or dilation/contraction frequency measured using the (complex-valued) Fourier transform of the response profile over time at each voxel is closely related to the polar angle or eccentricity
2 p. 2 Figure 1. Isoeccentricity and isopolar angle maps of human visual areas. The top row shows isoeccentricity coded by color (red [fovea] blue green [parafoveal] yellow red [periphery]) displayed on the original cortical surface (A), the unfolded cortical surface (B), and the cut and flattened cortical surface (C) (sulci. The bottom row shows polar angle (red [upper vertical meridian] blue [horizontal meridian] green [lower vertical meridian]) plotted on the same three surfaces (D,E,F). Local eccentricity and polar angle were determined by considering the phase of the response to a slowly dilating ring or a slowly rotating hemifield at the dilation or rotation frequency. The unfolded representations in B and E were made by relaxing curvature while approximately preserving local area and local angles (sulcal cortex is dark gray and gyral cortex is light gray). The flattened representations in C and F were made with the same algorithm after cutting off the occipital lobe and making an additional cut in the fundus of the calcarine sulcus. represented at that cortical location (13). This technique results in high signal-to-noise ratios (because at any one point in time, approximately one half of each visual field map will be activated) yet provides fine spatial resolution. Common (for example, retinal) and between-area phase delays can be removed and examined by considering clockwise/counterclockwise rotation and expansion/contraction pairs (14, 15). Figure 1A shows a color plot of the response to a dilating ring on a medial view of the cortical surface of the brain of this subject (A.M.D.) (16). The hue of the color at each cortical surface point indicates the response phase, which is here proportional to the eccentricity of the local visual field representation. In Figure 1B, the cortical surface was unfolded. This process is similar to inflation of a crumpled balloon except that the surface has not been stretched. In Figure 1C, the occipital lobe region containing the activated area has been cut off, and the resulting approximately conical surface cut again along the fundus of the calcarine sulcus to allow it to be flattened completely (17). There is a systematic increase in eccentricity (red blue green yellow red) moving anteriorly along the medial wall of occipital cortex. Lines of isoeccentricity run approximately in the coronal plane, cutting across several areas, as shown below. Ventrally, the region showing substantial retinotopy extends almost to the anterior-posterior midpoint of the unfolded ventral temporal lobe. A parallel treatment of data from the rotating hemifield stimulus collected a few minutes later is shown in Figure 1D-E. The color again indicates the phase of the periodic response, which is now proportional to the polar angle of the local visual field representation. The picture of polar angle is more complex, alternating between vertical and horizontal meridians both dorsally and ventrally. The upper field vertical meridian is red, the horizontal meridian is blue, and the lower field vertical meridian is green. Several alternations between
3 p. 3 Figure 2. Analysis of data in Fig. 1 by visual field sign (mirror-image vs. non-mirror-image visual field representation). Mirror-image areas (yellow e.g., V1), and non-mirror-image areas (blue e.g., V2) are shown in a medial view on the folded (A) and unfolded surface (B) and in a ventral view, folded (C) and unfolded (D). The incision in the fundus of the calcarine is visible in (B). Ventral V1, V2, VP, and V4v (18), comprising four re-representations of the upper visual field, are visible below the incision while lower visual field V1 and V2 are visible above the incision. The complex folding pattern of the occipital lobe coupled with the weak correlation between sulci and areal boundaries underscores the need for an unfolded representation. red and blue stripes are visible ventrally while several alternations between green and blue stripes are visible dorsally. Mapping experiments in monkeys suggest that several additional re-representations of the lower visual field adjoin V1 dorsally including V2 (second visual area) and V3 (third visual area) while several re-representations of the upper visual field adjoin V1 ventrally including V2, VP (ventroposterior area), and V4v (V4 ventral) (18). In particular, we would expect vertical meridian representations at the dorsal and ventral V1/V2 border, the ventral VP/V4v border, and the dorsal V3/V4 border, and horizontal meridian representations near the fundus of the calcarine sulcus in V1, at the dorsal V2/V3 border, at the ventral V2/VP border, and at the anterior border of ventral V4v (4, 6, 7). Candidates for all of the borders are visible in Figure 1D-E. Mapping experiments in monkeys have also revealed a number of small visual areas beyond those mentioned so far (including PO, parietal-occipital area), which may help to explain the presence of several small patches of lower field dorsally as well as upper field ventrally. Isoeccentricity and isopolar angle maps define two independent coordinates of retinotopy. Areal borders in either one of these maps, however, are often subtle; isoeccentricity lines can extend straight across several areas while polar angle maps often show only a shallow maximum or minimum at the border of an area. For example, the red stripe at the ventral upper field vertical meridian border of V1/V2 actually extends across both V1 and V2. By contrast, the visual field sign technique (7) provides an objective means to draw borders between areas based on analyzing the local relation between the directions of the fastest rate of change in these two coordinates. Regions of the cortex that contain a retinotopic map, however distorted, can be divided into two categories when viewed from the cortical surface those that contain a mirror-image representation of the visual field (like V1) and those that contain a non-mirror-image representation of the visual field (like V2). This
4 p. 4 Figure 3. Visual field sign displayed on the completely flattened occipital cortex (brightness indicates significance of response). Upper visual field V1, V2, VP, and V4v and lower visual field V1, V2, and V3 are now all visible. There are several robustly responding non-mirror image regions anterior to dorsal V2 and V3 that may correspond in part to V3A and dorsal V4 (not labeled). Regions with dimmer coloration may represent the central fovea (20), the visual field beyond 12 degrees eccentricity, or may be less retinotopic. distinction is unlikely to be of any fundamental functional significance, but it provides a convenient way to draw borders between areas because adjoining areas often have the opposite visual field sign. It is a local measure that can be calculated for each small patch of cortex given dense retinotopic mapping data like those obtained here. A map of visual field sign is shown on the folded and unfolded surface in a medial view (Fig 2A,B) and in a ventral view (Fig. 2C,D) (19). V1 is now clearly outlined as a large mirror-image patch (yellow) divided by our incision at the fundus of the calcarine sulcus. V2 forms two non-mirror image patches (blue) dorsally and ventrally. Two more areas are visible ventral and anterior to ventral V2 mirror-image VP (yellow) and, finally, non-mirror image V4v (blue) İn Figure 3, the cortex has been completely flattened, exposing dorsal and lateral areas concealed in Figure 2. Dorsal V2 is adjoined anteriorly by a thin band of mirror-image V3 (yellow). Just ventral and anterior to V3, the visual field sign pattern degenerates into noise near the center-of-gaze representations of V1 and V2 likely the result of the difficulty of mapping foveal cortex with this technique (20). Dorsal and anterior to V3, there are additional non-mirror image areas (blue) containing both upper and lower visual field representations that may correspond in part to V3A and dorsal V4 (not labeled). Even further anteriorly, areas are less obviously modulated at the stimulus rotation or dilation/contraction frequency, indicating either that they are foveal (<0.5 deg), peripheral (>12 deg), or less well organized retinotopically. Similar results were obtained in 6 other subjects. The areas revealed in these experiments show a number of similarities to areas originally discovered in non-human primates. A schematic comparison of human visual areas with macaque monkey visual areas (21) and owl monkey visual areas (7) is shown in Figure 4. At the top, the three flattened cortices are drawn at the same absolute scale while at the bottom, they are approximately scaled by the area of V1. It has long been known that V1 in humans is shifted medially around the occipital pole when compared to monkeys. The larger size of some human extrastriate areas relative to human V1 may have partially compensated for this shift [see e.g., the width of VP in Fig. 4B, the region between V2 and MT in (22)]; retinotopic areas extend nearly to the anterior-posterior midpoint of the ventral temporal lobe, just as they do in non-human primates. The anterior extent of retinotopic visual areas is most striking in the unfolded ventral view (Fig. 2D). Comparisons with the folded ventral view (Fig. 2C) show that more cortex is hidden in the posterior folds of the ventral occipital lobe than in the more anterior ventral temporal fissures. The internal structure of a visual cortical map can be characterized using the linear cortical magnification factor, M(r) mm of cortex per deg of visual angle as a function of eccentricity, r (23). We estimated the value of the parameters in a standard equation for magnification factor by measuring eccentricity on the cortical surface parallel to the average direction of fastest change of eccentricity in each upper and lower visual field representation described above. The resulting measurements were fit with a cortical mapping function, D(r) the distance on the cortex as a function of eccentricity (the integral of the magnification factor equation) by
5 p. 5 Figure 4. Schematic summary of retinotopic visual areas in the owl monkey (7), the macaque monkey (21), and the human (present study) at the same scale in (A) and approximately normalized by the area of V1 in (B) (human V1 is twice the area of macaque V1, with larger ocular dominance columns and cytochrome oxidase blobs, but a similar number of cells). Visual areas in humans show a close resemblance to visual areas originally defined in monkeys. The anterior border of visual cortex in humans was estimated using the superior temporal sulcus and intraparietal sulcus as landmarks. In (C), the mapping functions (scale on left axis) and magnification factor functions (scale on right axis) are shown for the upper field representations of human V1, V2, VP and V4 (24). The V1 mapping functions for owl monkeys (OM*, dotted) and macaque monkeys (MM*, dashed) shown at the left were scaled up to match the overall size of human V1 (25). An increased emphasis on the center of gaze in human V1 is evident. adjusting the parameters (24). Figure 4C shows the data and estimated mapping functions (points and heavy lines) and corresponding cortical magnification factor functions (light lines) for the upper field representations in human V1, V2, VP, and V4v. Human visual areas show a prominent emphasis on central vision, as reflected in the steepness of the mapping function, which corresponds to a large cortical magnification factor near the center of gaze. To compare these results with those from non-human primates, the mapping functions for macaque monkey and owl monkey V1 were first scaled to compensate for the differences in the overall size of V1 (human V1 is approximately twice the area of macaque V1 and about six times the area of owl monkey V1) (25). The resulting scaled mapping functions are shown in the leftmost graph in 4C. The macaque (dashed) and owl monkey (dotted) curves are considerably less steep than the human curve, indicating that human visual areas have an extreme emphasis on the center of gaze surpassing that seen not only in the nocturnal owl monkey but also that in the diurnal macaque monkey (26). It remains to be seen whether this will be explained by an increased emphasis on the center of gaze in the retina, in the retinogeniculocortical projection, or in both (27). Much has been made of the changes in areas beyond primary cortex in humans in comparisons with non-human primates. It is now apparent that
6 p. 6 human primary visual cortex is distinct as well. These studies of retinotopy in humans provide a framework for understanding the results of experiments designed to examine cortical responses to more complex and meaningful stimuli such as pictures, words, scenes, and sentences. It is interesting to note that several of the foci identified in previous non-invasive and invasive studies of responses to complex stimuli such as words (28) may overlap retinotopically organized areas already known from non-human primates. The techniques used here could be straightforwardly adapted to map tonotopy and amplitopy in auditory cortex, and somatotopy in somatosensory cortex. REFERENCES AND NOTES 1. M.I. Sereno and J.M. Allman, in The Neural Basis of Visual Function, A.G. Leventhal Ed. (Macmillan, London, 1991), pp ; J.H. Kaas and L.A. Krubitzer, Neuroanatomy of Visual Pathways and their Retinotopic Organization, B. Dreher and S.R. Robinson Eds. (Macmillan, London, 1991), pp ; D.J. Felleman and D.C. Van Essen, Cereb. Cortex 1, 1 (1991); M.G.P. Rosa, J.G. Soares, M. Fiorani Jr, R. Gattass, Vis. Neurosci. 10, 827 (1993). 2. D.C. Van Essen and S.M. Zeki, J. Physiol. (Lond.) 277, 193 (1978); D.C. Van Essen and J.H. Maunsell, J. Comp. Neurol. 191, 255 (1980). 3. R. Gattass, A.P.B. Sousa, C.G. Gross, J. Neurosci. 8, 1831 (1988). 4. R.B.H. Tootell, M.S. Silverman, R.L. DeValois, Science 214, 813 (1981); C.G. Cusick, H.J. Gould, J.H. Kaas, J. Comp. Neurol. 230, 311 (1984); R.B.H. Tootell, S.L. Hamilton, M.S. Silverman, J. Neurosci. 5, 2786 (1985); J. Olavarria and R.C. Van Sluyters, J. Neurosci. Meth. 15, 191 (1985); L.A. Krubitzer and J.H. Kaas, Vis. Neurosci. 5, 165 (1990). 5. P.T. Fox, F.M. Miezin, J.M. Allman, D.C. Van Essen, and M.E. Raichle, J. Neurosci. 7, 913 (1987); S. Zeki et al., J. Neurosci. 11, 641 (1991); W. Schneider, D.C. Noll, J.D. Cohen, Nature 365, 150 (1993). 6. W.T. Newsome, J.H.R. Maunsell, D.C. Van Essen, J. Comp. Neurol. 252, 129 (1986); D.J. Felleman, J.J. Knierim, D.C. Van Essen, Soc. Neurosci. Abstr. 12, 1182 (1986); R. Desimone and L.G. Ungerleider, J. Comp. Neurol. 248, 164 (1986); D.R. Boussaoud, R. Desimone, L.G. Ungerleider, J. Comp. Neurol. 306, 554 (1991); S. Neuenschwander, R. Gattass, A.P.B Sousa, M.C.G.P. Piñon, J. Comp. Neurol. 340,65 (1994). 7. M.I. Sereno, C.T. McDonald, J.M. Allman, Cereb. Cortex 4, 601 (1994); M.I. Sereno, C.T. McDonald, J.M. Allman, Cereb. Cortex 5, (1995, in press). 8. S.A. Engel et al., Nature 369, 525 (1994); E.A. DeYoe, P. Bandettini, J. Neitz, D. Miller, P. Winans, J. Neurosci. Meth. 54, 171 (1994). 9. J.W. Belliveau et al., Science 254, 716 (1991); K.K. Kwong et al., Proc. Nat. Acad. Sci. (USA) 89, A.M. Dale, M.I. Sereno, J. Cog. Neurosci. 5, 162 (1993). 11. Echo-planar images were collected on a 1.5 T scanner (GE Signa) with full body gradient coils (Advanced NMR) using an asymmetric spin echo sequence ( τ = -25 msec, TE=70 msec, TR= msec) [G.L. Wismer et al., J. Comp. Assist. Tomogr. 12, 259 (1988); J.R. Baker et al., 12th Ann. Proc. Soc. Mag. Res. Med., 1400 (1993); R.B.H. Tootell et al., J. Neurosci. (1995, in press)]. A 5-inch receive-only surface RF coil or a receive-only wrap coil was positioned near the occipital pole contiguous oblique 4 mm slices (voxel size: mm) were chosen to lie approximately perpendicular to the calcarine sulcus. Before and after the set of functional scans for a subject, we recorded a T1-weighted series of echo-planar images (spin echo inversion recovery sequence: TE=40 msec, TI=1050 msec, TR=20000 msec, NEX=2) with the same orientation, slice thickness, in-plane resolution, and field of view as the functional scans. We used the T1 series to align the functional scans with the higher resolution structural scan (voxel size: mm) used for surface reconstruction that were collected in a separate session using a head coil. 12. The visual stimuli were generated in real time on a Silicon Graphics Onyx computer using GL graphics library functions. The high resolution RGB video output signal was subsampled and converted to a composite video signal that was used to drive a Sony 2000 color LCD projector. Informed consent to these experiments was obtained from subjects, several of whom were also authors (M.I.S., A.M.D., R.B.H.T.). Supine subjects looked up into an adjustable angled mirror that allowed them to comfortably view a frosted back-projection screen arranged perpendicular
7 p. 7 to the bore just below their chin. Residual head movements were controlled though the use of a dental impression bite bar made before the scan for each subject and supported by an adjustable plastic yoke. Care was taken to block subject s direct view of the screen. Subjects were given the opportunity to take ibuprofen ( mg) before the scan as a prophylactic against the minor discomforts that typically accompany attempts to remain very still for extended periods of time. Images were projected onto the screen through a collimating lens and subtended a maximum visual angle 35 deg wide and 26 deg tall. Stimuli consisted of black and white checkerboard patterns counterphase flickering at 4 Hz (i.e., one cycle consists of 1/8 sec of black and 1/8 sec of white), which is near the optimal temporal frequency for driving cortical neurons [(5); K.H. Foster, J.P. Gaska, M. Nagler, D.A. Pollen, J. Physiol. 365, 331 (1985)]. The checkerboard patterns were scaled with eccentricity. These patterns stimulated a circle in the visual field with a radius of degrees. The ring and hemifield stimuli were designed to activate approximately half of the ganglion cells in the central degrees of the two retinae at any one point in time. 13. The time series of activation (across the 128 images of each slice) was examined on a pixel-by-pixel basis. The linear trend and baseline offset for each pixel time series was first removed by subtracting off a line fitted through the data by least-squares. The discrete Fourier transform of the time series for each pixel was then computed to give 128 complex values. In retinotopically organized areas, the amplitude spectrum showed a sharp peak at the stimulus rotation or dilation/contraction frequency (~0.015 Hz) 5-30 times larger than peaks at other frequencies. The phase angle of the response at the stimulus rotation (or dilation/contraction) frequency at a voxel is related to the polar angle (or eccentricity) represented there. The phase angles for the pixels in a slice were then corrected to take account of delays resulting from the known order in which the slices were collected (1,3,5...2,4,6...). Finally, the phase angles were mapped to different hues whose intensity was a function of the ratio between the amplitude at the stimulus frequency and the average amplitude of all other frequencies (this ratio can reach in V1). Our basic procedure is closely related to correlation of the signal with a sinusoid [cf. P.A. Bandettini et al., Mag. Res. Med. 25, 390 (1992); P.A. Bandettini, A. Jesmanowicz, E.C. Wong, J.S. Hyde, Mag. Res. Med. 30, 161 (1993)]. 14. In general, the phase of the periodic response will be delayed due to finite vascular response time. The basic stimulus frequency was low enough so that there was no whole-cycle phase ambiguity. Residual phase delays were canceled by considering the circular average of the phase angles obtained for opposite directions of stimulus motion (contraction vs. expansion, clockwise vs. counterclockwise) at each voxel after reflecting the phase angles for the opposite stimulus direction around We rejected scans in which substantial movement (~2 mm) had occurred. This was easily recognized by viewing animations of the 128 images for each slice. Nevertheless, even in the presence of such movements, a sharp peak at the basic stimulus frequency (~0.015 Hz) was usually larger than the lower frequency peaks due to movement. Note that we have discretely sampled a continuous function the intensity of a given voxel over time. Since that signal has not been explicitly limited in bandwidth before sampling, there is also the danger that frequencies higher than the Nyquist 1 critical frequency ( f c Hz for TR= ms) could 2 alias back into the spectrum we intended to measure. Changes in the signal due to blood oxygenation are unlikely to be fast enough to cause such a problem. Artifactual signals due to brain motion caused by rapid head motion were controlled through the use of a bite bar. Brain movement artifacts induced by cardiac pulsation are potentially more problematic; however, there is enough variation in frequency and phase of the cardiac signal to avoid the generation of large aliased peaks in the Fourier amplitude spectrum given the number of stimulus cycles used in the present study. 16. To paint the functional data onto the cortical surface, blink comparison in three orthogonal planes was first used to align the echo planar inversion recovery images (3 3 4 mm taken in the plane of the functional images) with the high resolution data set (1 1 1 mm) used to reconstruct the cortical surface (17). The functional data set was then sampled with the cortical surface. By using a surface nearer the gray/white matter border than the pial surface, we were able to accurately assign activations to the correct bank of a sulcus despite the fact that the individual functional
8 p. 8 voxels were comparable in size to the thickness of the cortex. Our success in this endeavor is demonstrated by the lack of ambiguity in recovering the closely apposed upper and lower visual field representations situated on opposite sides of the calcarine sulcus. The lower resolution activation data (1 sample 3 3 mm) was smoothly interpolated onto the high resolution surface reconstruction (1 polygon 1 1 mm). 17. The folded, unfolded, and flattened surfaces were made from high resolution T1-weighted images (1 1 1 mm) optimized for gray/white matter contrast using techniques similar to those presented in (10) (cf. E.L. Schwartz, in Computational Neuroscience, E.L. Schwartz, Ed. (Wiley, New York, 1990), pp , and G.J. Carman, thesis, California Institute of Technology (1990)). The skull was first automatically stripped off by shrink-wrapping a stiff deformable template onto the brain. The gray/white matter boundary for each hemisphere was then estimated with a region-growing method. The result was tessellated to generate a surface (~150,000 vertices) that was refined against the MRI data using a deformable template algorithm, inspected for topological defects (e.g., handles ), and re-made if necessary. To obtain a completely flattened cortical surface, the occipital lobe was cut off and the fundus of the calcarine incised by disconnection of vertices. The resulting surface fragment was then pushed onto a coronal plane in one step and unfurled on the plane. The vertex update rule was modified from that in (10) to include local area-preserving and shear-minimizing terms. Beautiful images of the cortical surface can be generated by rendering stacked slices [H. Damasio and R. Frank, Arch. Neurol. 49, 137 (1992)]. Such images, however, lack explicit information about cortical surface orientation and connectivity required for cortical unfolding. It is possible to trace the cortical ribbon in individual slices and manually connect them into a surface [M.L. Jouandet et al., J. Cog. Neurosci. 1, 88 (1989)] but these techniques are difficult to implement in regions where sulci run nearly parallel to slices as they do in any slice plane through the occipital lobe. 18. Area VP has sometimes been labeled V3v (ventral V3) while area V4v has sometimes been labeled VA (ventroanterior area). More definitive statements of homology await future studies of the functional properties of these retinotopically defined regions in humans. 19. The gradients in retinal eccentricity and polar angle with respect to cortical x and y, r and θ, are vector quantities whose norms have units deg/mm (the reciprocal of magnification factor). They were computed by fitting a plane to the r (or θ) values of the current vertex and its immediate neighbors using least squares. The clockwise angle, λ, between r and θ was then measured to determine whether the local representation of the visual field at that vertex was non-mirror-image (λ near π/2) or mirror-image (λ near π/2). Finally, the intensity of the field sign coloring was adjusted using the average significance from the eccentricity and polar angle data sets. 20. The limited resolution of the video projector made it difficult to present checkerboard patterns scaled with eccentricity near the center of gaze while still covering a reasonable amount of visual angle peripherally. Small imperfections in fixation also have a much more deleterious effect at the center of gaze than they do in the near periphery. In order not to occlude the fixation cross, the central 0.5 deg of the ring and semicircle stimuli were omitted. These considerations lead us to expect the periodic signal to fall off in the foveal parts of the visual field. This region of the visual field would be expected to be represented across several cm 2 of cortex just anterior to the occipital pole on the lateral surface of the brain. Mapping this region would require higher resolution stimuli and additional averaging to overcome fixation jitter. 21. D.C. Van Essen, C.H. Anderson, D.J. Felleman, Science 255,419 (1992). 22. J.D. Watson et al., Cereb. Cortex 3, 79 (1993); R.B.H. Tootell and J.B. Taylor, Cereb. Cortex 5, 39 (1995). 23. R.B.H. Tootell, M.S. Silverman, E. Switkes, R.L. DeValois, Science 218, 902 (1982); D.C. Van Essen, W.T. Newsome, J.H. Maunsell, Vis. Res. 24, 429 (1984); D.J. Tolhurst and L. Ling, Hum. Neurobiol. 6, 247 (1988); J.C. Horton and W.F. Hoyt, Arch. Ophthalmol. 109, 816 (1991); E.L. Schwartz, in Cerebral Cortex, Vol. 10, Primary Visual Cortex in Primates, A. Peters and K.S. Rockland, Eds. (Plenum, New York, 1994), pp The falloff in linear cortical magnification factor, M, (mm of cortex per deg of visual angle) with increasing eccentricity has often been described using an equation of the form:
9 p. 9 M( r) = A [ r + B] C (23), where r is the eccentricity, and A, B, and C are constants (with C sometimes constrained to be 1). To estimate M(r), activated regions (vertices) of the flattened visual field sign map were first marked by visual area and by whether they contained upper or lower field representations, omitting regions of ambiguous visual field sign. The average direction of the cortical eccentricity gradient (vector sum of r across every vertex assigned to an area) was estimated independently for each upper and lower visual field representation. The mapping function, D( r) = M( r) dr, where D(r) is the distance in mm on the cortex from the center of gaze, was determined for each area by measuring distances from the most central response zone (representing approximately 0.5 deg eccentricity) along the direction of the average eccentricity gradient for each labeled vertex. The measurements were combined into 30 eccentricity bins. The resulting points were then fit with the equation for the mapping A ( r + B) 1 C function, D( r) = M ( r) dr =, C 1 by 1 C adjusting the parameters A, B, and C. The resulting cortical magnification factor equations for human upper visual field V1, V2, VP, and V4 were: M V1 (r) = [r ] ; M V2 (r) = [r ] ; M VP (r) = [r ] ; M V4v (r) = [r ] Magnification factor at a particular eccentricity will be proportional to the size of V1 if the shape of the mapping function (cortical distance vs. eccentricity) does not change. To compare the mapping function for humans to that for owl monkeys and macaque monkeys, the mapping functions for those animals were first scaled up to a human-sized V1 using values for B and C from the literature (23). The resulting equations for cortical magnification factor were: M OM* (r) = [r + 2.5] -1.0 ; M MM* (r) = [r ] Cortical magnification factor equations are sometimes constrained to have C = 1, which results in a particularly simple mapping function: D(r) = A log[r + B]. This equation fits non-human primate data quite well. Our data could also be fit with this equation, but only if we allowed B to be negative, which results in a singularity (infinite magnification factor) before the center of gaze is reached. A good fit without a singularity could only be achieved with C above 1. The combinations of parameters given here fit the cortical distance data very closely but still give unrealistically large estimates of cortical magnification at the exact center of the fovea (extrapolation of the dotted portion of cortical magnification curve in Fig. 4C), indicating that the standard equation for M is inadequate to accurately describe cortical magnification in the very center of the fovea in humans even with C > 1. The data presented in (8) are consistent with ours in that D(r) is almost vertical near the center of gaze; accurately fitting their cortical distance data at 2-10 deg eccentricity will give equally extreme estimates of cortical magnification at the exact center of gaze. 27. It is possible that differences at the level of the human retina (and/or LGN) may partly account for the differences in cortical magnification factor we observed. For example, human OFF midget retinal ganglion cells have dendritic fields that are 30% smaller in diameter than their ON counterparts a contrast not seen in the macaque monkey retina [D.M. Dacey, J. Neurosci. 13, 5334 (1993)]; and the fibers of Henle are especially long in the human retina [C.A. Curcio, K.A. Allen, J. Comp. Neurol. 300,5 (1990)]. These observations are consistent with an increase in the foveal density of human midget ganglion cells with respect to macaque monkeys, which could explain our result. 28. S.E. Petersen, P.T. Fox, A.Z. Snyder, M.E. Raichle, Science 249, 1041 (1990); A.C. Nobre, T. Allison, G. McCarthy, Nature 372, 260 (1994). 29. We thank Marta Kutas, Rick Buxton, Lourdes Anllo-Vento, and Giorgio Ganis at UC San Diego, Tim Davis, John Baker, Chantal Stern, Randall Benson, Terrence Campbell, and Mike Vevea at the MGH NMR Center, Steve Engel, Brian Wandell, and David Rumelhart at Stanford, Ted DeYoe and Eric Wong at Medical College of Wisconsin, John Allman at Caltech, and Dennis Dacey at University of Washington for help, comments, and discussions. Supported by ONR N , the UCSD McDonnell-Pew Cognitive Neuroscience Center, the Norwegian Research Council, NIH grants MH47035, NICHD22614 (Marta Kutas), EY07980, MH50054, HL39810, P01 CA48729, and by the Human Frontier Science Program.
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