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The Journal of Neuroscience, December 1, 1998, 18(23):10053-10069
Red, Green, and Red-Green Hybrid Pigments in the Human Retina:
Correlations between Deduced Protein Sequences and Psychophysically
Measured Spectral Sensitivities
Lindsay T.
Sharpe1,
Andrew
Stockman2,
Herbert
Jägle1,
Holger
Knau1,
Gert
Klausen3,
Andreas
Reitner4, and
Jeremy
Nathans5
1 Forschungsstelle für Experimentelle
Opthalmologie, Universitäts-Augenklinik Abteilung II, D-72076
Tübingen, Germany, 2 Department of Psychology,
University of California San Diego, La Jolla, California, 92093-0109, 3 Neurologische Universitätsklinik, D-79106 Freiburg
im Breisgau, Germany, 4 Universitäts Augenklinik,
1090 Vienna, Austria, and 5 Departments of Molecular
Biology and Genetics, Neuroscience, and Ophthalmology, Howard Hughes
Medical Institute, Johns Hopkins University School of Medicine,
Baltimore, Maryland 21205
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ABSTRACT |
To analyze the human red, green, and red-green hybrid cone
pigments in vivo, we studied 41 male dichromats, each of
whose X chromosome carries only a single visual pigment gene
(single-gene dichromats). This simplified arrangement avoids the
difficulties of complex opsin gene arrays and overlapping cone spectral
sensitivities present in trichromats and of multiple genes encoding
identical or nearly identical cone pigments in many dichromats. It thus allows for a straightforward correlation between each observer's spectral sensitivity measured at the cornea and the amino acid sequence
of his visual pigment. For each of the 41 single-gene dichromats we
determined the amino acid sequences of the X-linked cone pigment as
deduced from its gene sequence. To correlate these sequences with
spectral sensitivities in vivo, we determined the Rayleigh matches to different red/green ratios for 29 single-gene dichromats and measured psychophysically the spectral sensitivity of
the remaining green (middle wavelength) or red (long wavelength) cones
in 37 single-gene dichromats. Cone spectral sensitivity maxima obtained
from subjects with identical visual pigment amino acid sequences show
up to a ~3 nm variation from subject to subject, presumably because
of a combination of inexact (or no) corrections for variation in
preretinal absorption, variation in photopigment optical density,
optical effects within the photoreceptor, and measurement error. This
variation implies that spectral sensitivities must be averaged over
multiple subjects with the same genotype to obtain representative
values for a given pigment. The principal results of this study are
that (1) ~54% of the single-gene protanopes (and ~19% of all
protanopes) possess any one of several 5'red-3'green hybrid genes that
encode anomalous pigments and that would be predicted to produce
protanomaly if present in anomalous trichromats; (2) the alanine/serine
polymorphism at position 180 in the red pigment gene produces a
spectral shift of ~2.7 nm; (3) for each exon the set of amino acids
normally associated with the red pigment produces spectral shifts to
longer wavelengths, and the set of amino acids normally associated with
the green pigment produces spectral shifts to shorter wavelengths; and
(4) changes in exons 2, 3, 4, and 5 from green to red are associated
with average spectral shifts to long wavelengths of ~1 nm (range,
0.5 to 2.5 nm), ~3.3 nm (range, 0.5 to 7 nm), ~2.8 nm (range,
0.5 to 6 nm), and ~24.9 nm (range, 22.2-27.6 nm).
Key words:
visual pigments; cone pigments; red-green color
blindness; spectral sensitivity; human retina; protein sequences
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INTRODUCTION |
Normal human color vision is
mediated by three light-sensitive cone photopigments.a Two of
these, the red pigment and the green pigment, are encoded by highly
homologous genes that reside in a head-to-tail tandem array on the X
chromosome (for review, see Nathans et al., 1992 ). The common variants
of red-green color vision arise from unequal homologous exchanges
within this gene array that cause a loss of one of the two types of
visual pigment genes and/or the production of hybrid genes. Simple loss
of one of the X-linked pigments produces dichromacy, whereas
replacement of one of the X-linked pigments with a hybrid pigment
results either in dichromacy or anomalous trichromacy, depending on the
extent to which the absorbance spectrum of the hybrid pigment differs
from that of the remaining normal pigment.
Two factors complicate the interpretation of genotype-phenotype
correlations in the study of red-green color vision. First, the number
of visual pigment genes within an array varies among X chromosomes. In
general, each visual pigment gene array has only a single red pigment
gene, whereas the number of green pigment genes varies from one to at
least five (Nathans et al., 1986a ; Drummond-Borg et al., 1989 ; Macke
and Nathans, 1997 ; Yamaguchi et al., 1997 ) [although see Neitz and
Neitz (1995) and Neitz et al. (1995a) for a dissenting view]. The
presence of more than one green pigment gene, or in the case of
deuteranomalous trichromats (subjects with an altered green cone
sensitivity; abbreviated here G'R+) more than one
5'green-3'red hybrid gene and/or green pigment gene, complicates the
correlation of genotype and phenotype because recent evidence indicates
that only a subset of the green pigment genes is expressed (Winderickx
et al., 1992b ; Yamaguchi et al., 1997 ). There is currently no method
for determining from the genotype which green or 5'green-3'red hybrid
pigment genes are expressed in those individuals who carry multiple
copies of these genes in their array. A second complication arises from
the observation that single nucleotide polymorphisms create variant
pigments in which spectral sensitivity may be shifted by as much as
~5 nm. One of the most common polymorphic variations occurs at codon 180 in the red pigment gene where site-directed mutagenesis experiments suggest that the presence of an alanine or a serine results in a shift
to shorter or longer wavelengths, respectively, of ~4 nm (Merbs and
Nathans, 1992a ) or 2-7 nm (Asenjo et al., 1994 ) (also see below). The
exact spectral shifts referable to this and other polymorphisms are of
considerable interest because these sequence differences are likely to
account for much of the variation in color vision between normal trichromats.
Experiments aimed at defining the cone spectral sensitivities that
underlie both normal and anomalous color vision have been pursued for
over a century. One approach has been to use psychophysical techniques
that isolate single cone sensitivities in vivo by exploiting the selective desensitization caused by either steady (Stiles, 1939 ,
1964 ; De Vries, 1948a ,b ; Wald, 1964 ) or transient (Stockman et
al., 1993b ) chromatic adaptation. With these techniques it is possible
to isolate the red and green cones of normals throughout the spectrum
(Stockman et al., 1993a ,b ) and the blue cones from short wavelengths to
~540 nm (Stiles, 1953 ; . However, the
psychophysical isolation of cones containing red-green hybrid pigments
from the accompanying normal red or green cones has been difficult or
impossible to achieve in X chromosome-linked anomalous trichromats,
owing to the similarities between the spectral sensitivities of these pigments (see Stockman et al., Piantandida and Sperling, 1973a ,b ; Pokorny et al., 1973 ;
Rushton et al., 1973b ).
The simplest and most commonly used method for isolating the red or
green cone sensitivities is to study red-green dichromats who lack
either red or green cone photopigments (Pitt, 1935 ; Hecht, 1949 ;
Willmer, 1950 ; Hsia and Graham, 1957 ; Mitchell and Rushton, 1971 ;
Rushton et al., 1973a ; Smith and Pokorny, 1975 ). On the assumption that
their color vision is a "reduced" form of normal color vision
(Maxwell, 1860 ; König and Dieterici, 1886 ), that is, that their
surviving cones have the same spectral sensitivities as their
counterparts in color-normal trichromats, these data have been used to
define normal cone spectral sensitivities. Not all dichromats, however,
conform to the reduction hypothesis, either because they have hybrid
photopigments or because they have multiple photopigment genes (Nathans
et al., 1986b ; Deeb et al., 1992 ). Only red-green dichromats with a
single normal photopigment gene or with multiple genes that produce
identical photopigments will conform completely to the reduction
hypothesis. This recently appreciated genetic complexity calls into
question the conclusions of previous studies in which the genotypes of the red-green dichromats were unknown.
Over the past several decades the techniques of fundus reflectometry
(Rushton, 1963 , 1965 ), microspectrophotometry (Dartnall et al., 1983 ),
single-cell electrophysiology (Schnapf et al., 1987 ), and
electroretinography (Neitz et al., 1995b ) also have been applied
to the study of human cone pigment spectral sensitivities. The most
recent approach to this problem has come from the in vitro
study of recombinant cone pigments produced in tissue culture cells
(Oprian et al., 1991 ; Merbs and Nathans, 1992a ,b ; Asenjo et al., 1994 ).
These experiments have defined the absorption properties of the normal
cone pigments, their common polymorphic variants, and each of the
several hybrid pigments that underlie anomalous trichromacy. However,
the reported measurements of visual pigment absorbance in solution
suffer from two limitations: they are only accurate within
approximately one log unit of the peak absorbance and thus encompass
only a limited range of wavelengths, and they differ from measurements
in the living eye owing, for example, to waveguiding (Enoch, 1961 ,
1963 ) and to self-screening (Brindley, 1953 ) effects in the cone photoreceptor.
To analyze red, green, and red-green hybrid pigments in vivo
while avoiding the difficulties of complex opsin gene arrays and
overlapping cone spectral sensitivities, we have chosen to study male
dichromats each of whose X-chromosome carries only a single visual
pigment gene. This simplified arrangement allows for a straightforward
correlation to be made between spectral sensitivity and the
individual's visual pigment sequence, and it eliminates problems
associated with dichromats who carry multiple genes that may differ
subtly in spectral sensitivity. In this paper we report the spectral
sensitivities of red, green, and 5'red-3'green hybrid pigments
determined in the living human eye by psychophysical methods, together
with the amino acid sequences of the corresponding proteins as deduced
from their gene sequences. The results permit a direct correlation
between single amino acid substitutions and in vivo shifts
in spectral sensitivity in both normal and anomalous pigments.
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MATERIALS AND METHODS |
Human subjects. Males with severe color vision
deficiencies were recruited in Freiburg, Tübingen, and Vienna via
word of mouth and by advertising in local newspapers and cinemas. Most subjects were native Germans or Austrians; ~15% of subjects were natives of the Balkan peninsula. Subjects were between 16 and 45 years
old, with a mean age of 28. Their ages are given in Tables 3 and 4. To
identify and classify the dichromats within this group, we examined the
subjects by anomaloscopy as described below.
Genotyping. Venous blood samples were obtained from 94 dichromat subjects, and genomic DNA was purified by proteinase K
digestion and equilibrium centrifugation in cesium chloride. Southern
blots of BamHI and EcoRI-digested DNA were probed
with a 350 bp EcoRI-BamHI fragment from the 5'
end of a full-length human red pigment cDNA clone (hs7; Nathans et al.,
1986a ) to visualize two restriction fragments from the green pigment
gene (referred to as Bg and Cg), and two
restriction fragments from the red pigment gene (referred to as
Br and Cr; Fig.
1B). Those DNA samples
that showed three or more hybridizing fragments must have two or more
visual pigment genes within the X chromosome. Those DNA samples with
only one version of fragment B and one version of fragment C were
presumed to carry a single visual pigment gene. In each Southern blot
pattern of this type, visual inspection of the hybridization intensity of the B and C bands showed that they corresponded to the lowest intensity level seen among all of the subjects, consistent with the
presence in these samples of only a single visual pigment gene. With
the use of primers in the flanking intron regions (Nathans et al.,
1993 ), exons 2-5 were amplified by PCR from each of the 41 DNA samples
that were presumed to carry a single visual pigment gene, together with
four samples predicted to carry more than one visual pigment gene. The
PCR products were purified by absorption to an affinity column (Qiagen,
Hilden, Germany), and both strands were sequenced by the use of
thermocycle sequencing with fluorescent chain terminators (Applied
Biosystems, Foster City, CA).

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Figure 1.
Homologous recombination between red and
green pigment genes in dichromat subjects. A, Schematic
diagram of unequal homologous recombination between the most 5' gene in
one visual pigment gene array (a red pigment gene) and the most 3' gene
in a second visual pigment gene array (a green pigment gene). For
simplicity, only one of the usually multiple green pigment genes is
shown in each of the wild-type arrays. Recombination events within the
coding regions produce an array with a single 5'red-3'green hybrid gene
(crossover 1), resulting in a
G+R or a
G'R phenotype; recombination events 3' to the
coding regions produce an array with a single red pigment gene
(crossover 2), resulting in a
G R+ phenotype.
B, Diagram of the red and green pigment genes showing
the locations of the six exons and the
BamHI-EcoRI restriction fragments
Bg and Cg (derived from the green pigment gene)
and Br and Cr (derived from the red pigment
gene). The B fragments encompass 5' flanking DNA, exon 1, and part of
intron 1, and the C fragments encompass part of intron 1 and the 5'
half of exon 2 [see Nathans et al. (1986) for a detailed restriction
map]. C, Representative whole genome Southern blot
hybridization to identify dichromats with X chromosome visual pigment
gene arrays with only a single gene. A human red pigment cDNA
probe encompassing exon 1 and the 5' half of exon 2 (5' of the
BamHI site) was hybridized to a Southern blot of human
genomic DNA cut with both EcoRI and
BamHI. This probe hybridizes with equal efficiency to
the red and green pigment genes. In the Southern blot shown here,
HS2180, HS2183, HS2186, and HS2187 carry two or more X-linked visual
pigment genes as judged by the presence of both red and green versions
of fragments B and C. HS2181, HS2182, HS2184, and HS2185 are presumed
to carry a single visual pigment gene as judged by the presence of only
one version of fragment B and one version of fragment C.
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Rayleigh matches. X chromosome-linked (red-green) dichromacy
traditionally is established by Rayleigh matches. The subject must be
able to match fully a spectral yellow primary light to a juxtaposed
mixture of spectral red and green primary lights merely by adjusting
the intensity of the yellow, regardless of the red-to-green ratio. This
is consistent with quantal absorptions in a single photopigment being
responsible for the matches (the choice of the wavelengths and
intensities of the primaries as well as the field size mainly precludes
absorptions in the blue cones or rods from influencing the matches).
Subjects were tested for their Rayleigh matches on one or more of four
anomaloscopes: a König-Helmholtz colorimeter and a Nagel II
anomaloscope and two Nagel I anomaloscopes. Because they were recruited
and tested over a span of several years and at several locations, only
a subset of subjects was tested on all the instruments. The field of
view (2-2.6° in diameter) and the wavelengths and intensities of the
primary lights varied among the four anomaloscopes.
All the dichromat subjects listed in Tables 2-4 (n = 45) made repeated matches (three to five times) in random order for 17 different red-to-green mixture ratios solely by adjusting the intensity
of the yellow primary light. Their individual matching range slopes
(i.e., the slopes of regression lines fit to their yellow intensity
settings for the 17 red-green mixtures) and intercepts (i.e., the
yellow intensity required to match the red primary alone) then were
determined by a least-squares criterion. From the extent of the
matching range (i.e., whether the subjects could match both the red and
green primary lights) and the slope of the regression line, the
subjects were categorized as
G+R (protanopes),
G R+ (deuteranopes), or
anomalous trichromats (for classification details, see Pokorny et al.,
1979 ; Wyszecki and Stiles, 1982 ).
Flicker photometry: apparatus. A Maxwellian view optical
system produced the flickering test stimuli and the steady adapting field. All optical channels originated from a 75 W xenon arc lamp (Osram, Berlin, Germany) run at constant current. Two channels provided
the 2° in visual diameter flickering test and reference lights. Their
wavelengths were shaped by grating monochromators (H-10 Vis,
Jobin-Yvon, Longjumaneau, France) with 0.5 mm entrance and exit slits
into a triangular profile having a full bandwidth at half-maximum
(FWHM) of ~4 nm. The wavelength of the reference light was always set
to 560 nm, whereas that of the test light was varied from 400 to 700 nm
in 5 nm steps. At wavelengths longer than 560 nm a glass cutoff filter
(Schott OG550), which blocked short wavelengths but transmitted
wavelengths higher than 550 nm, was inserted after the exit slit of
both monochromators. This filter reduces the skirt of shorter
wavelength stray light. The third channel provided the 18° diameter
adapting field. The wavelength of the third channel was shaped by a
grating monochromator (Jobin-Yvon H-10 Vis) with 2 mm entrance and exit
slits into a triangular profile, peaking at 430 nm (FWHM = 17 nm).
Infrared radiation was eliminated by heat-absorbing glass (Schott,
Mainz, Germany) placed early in each beam.
The images of the xenon arc were <1.5 mm in diameter at the plane of
the observer's pupil. Circular field stops placed in collimated
portions of each beam defined the test and adapting fields as seen by
the observer. Mechanical shutters driven by a computer-controlled
square-wave generator were positioned in each channel near focal points
of the xenon arc. The optical waveforms so produced were monitored
periodically with a Pin-10 diode (United Detector Technology, Santa
Monica, CA) and oscilloscope.
Fine control over the luminance of the stimuli was achieved by variable
2.0 log unit linear (Spindler and Hoyer) or 4.0 log unit circular
(Rolyn Optics) neutral density wedges positioned at image points of the
xenon arc lamp and by insertion of fixed neutral density filters in
parallel portions of the beams. The position of the observer's head
was maintained by a rigidly mounted dental wax impression.
Flicker photometry: calibration. The radiant fluxes of the
test and adapting fields were measured at the plane of the observer's pupil with a calibrated radiometer (Model 80X Optometer, United Detector Technology) or with a Pin-10 diode connected to a picoammeter (Model 486, Keithley, Taunton, MA). The calibration of the silicon detector was checked against a similar model (now produced by Graseby),
both of which had been calibrated by the manufacturers against
standards traceable to the National Bureau of Standards, USA. In
addition, the UDT radiometer was checked against a photodiode that was
calibrated against the German national standard (Braunschweig). The
fixed and variable neutral density filters were calibrated in
situ for all test and field wavelengths. Particular care was taken
in calibrating the monochromator and interference filters: spectroradiometers were used to measure the center wavelength and the
FWHM at each wavelength in the experiments conducted in Freiburg,
Germany (Spectra Scan, Photo Research) and Tübingen, Germany
(Instrument Systems).
The radiometric accuracy of the calibrations was better than 0.01 log
unit from 400 to 700 nm, whereas the resolution of the individual
settings was better than 0.02 log unit. The absolute wavelength
accuracy was better than 0.5 nm (Freiburg) or 0.2 nm (Tuebingen),
whereas the resolution of the wavelength settings was better than 0.15 nm.
Spectral sensitivity measurements. Corneal spectral
sensitivities were measured by heterochromatic flicker photometry. The measurements were confined to the central 2° of the fovea. A
reference light (560 nm) was alternated at a rate of 16 or 25 Hz, in
opposite phase with a superimposed test light, the wavelength of which was varied in 5 nm steps over the spectrum from 400 to 680 nm. In some
subjects the shorter and longer wavelength regions were measured during
separate runs. To saturate the rods and to prevent the blue cones from
contributing to spectral sensitivity, we superimposed the flickering
stimuli on a large violet (430 nm) background with an intensity of 11.0 log quanta · sec 1 · degree 2, which is more than one log unit above rod saturation.
At the start of the spectral sensitivity experiment, the subject
adjusted the intensity of the 560 nm reference flickering light until
he was satisfied that the flicker was just at threshold. After five
settings had been made, the mean threshold setting was calculated and
the reference light was set 0.2 log unit above this value. Then the
test light was added to the reference light in counterphase. The
subject adjusted the intensity of the flickering test light until the
flicker percept disappeared or was minimized. This procedure was
repeated five times at each wavelength. After each setting the
intensity of the flickering test light was randomly reset to a higher
or lower intensity so that the subject had to readjust the intensity to
find the best setting. The target wavelength was varied randomly in 5 nm steps from 400 to 700 nm. From two to six complete runs were
performed by each subject. Thus, each data point represents between 10 and 30 threshold settings.
Analysis of flicker photometry data. Measurements were made
in naïve subjects. Consequently, although a majority of the
measurements were acceptable, a small minority were of doubtful
quality. To avoid distorting the max (wavelength of
maximal absorption) estimates, we adopted a standard method for
eliminating doubtful data points from the analysis. Because each data
point was averaged from five individual settings, its quality could be
judged from their SD. Figure
2A shows the frequency
of the SDs of the five settings for the data points for all observers.
To eliminate the most doubtful data, we rejected points for which the
SD of the five settings was >0.15 log unit. In terms of the frequency
distribution shown in Figure 2A, this cutoff is 2 SDs
higher than the mean and results in a rejection rate of 3.4%.

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Figure 2.
Elimination of unreliable data from the analysis.
A, Frequency of the SDs of the five individual settings
(in log units) averaged to produce each of the data points for
protanopes (open bars; 2410 data points) and
deuteranopes (filled bars; 3820 data points);
3.4% of the data points, the five settings of which had SDs > 0.15 log unit, were eliminated from the analysis. The SD axis is
truncated at 0.5 log unit. A few points had SDs higher than 0.5. B, Frequency of the log residuals between the data
points and the first fit of the spectral sensitivity model [see Eqs.
1, 2, and 3a for protanopes (open bars; 2290 points) and
deuteranopes (filled bars; 3730 points)]; 2.6%
of the data points, the residuals of which were >0.20 log unit, were
eliminated from the second fit of the model.
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Some data points had small SDs yet were clearly discrepant from the
surrounding points and from the predictions of the models described
below. They arose, we believe, because subjects occasionally did not
adjust the target radiance to find the appropriate flicker null. Figure
2B shows the frequency of the residuals between the data points (after the points with a high SD had been eliminated) and
the predictions of the full spectrum model (see below). To avoid the
discrepant points from distorting the max estimates (which is a problem particularly at longer wavelengths), we eliminated all data points for which the residuals were >0.20 log unit. In terms
of the frequency distribution shown in Figure 2B, the
cutoffs are 2.5 SDs above and below the mean, and they result in a
rejection rate of 2.6% (so that the cumulative rejection rate for both
steps was ~6%).
The max of each subject's red, green, or red-green
hybrid spectral sensitivity was estimated by fitting a photopigment
template to his flicker photometric data. The photopigment template was derived from the green and red cone spectral sensitivities of Stockman
et al. (1993a) . First, the Stockman et al. (1993a) green and red cone
spectral sensitivities were corrected individually to the retinal level
by removing the effects of macular and lens pigmentation. Next, they
were corrected to photopigment optical density (or absorbance) spectra
by adjusting them to infinitely dilute photopigment concentrations. The
assumptions required for these corrections are given in Stockman et al.
(1993a) , in which the red and green cone spectra also are illustrated
[Stockman et al. (1993a) , their Fig. 15, lower panel]. We next
derived a simple polynomial function to describe the logarithm of the
red and green cone photopigment spectra after the red cone spectrum had
been shifted horizontally along a log10 wavelength
[log( )] scale to align it with the green cone spectrum. The log
photopigment optical density spectrum,
log[POD(x)], normalized to zero
peak, is:
|
(1)
|
where x is log( ), a = 3593840.5764, b = 48574668.0585, c = 262378945.6275, d = 708007074.0766, e = 954435497.8303, f = 514228901.1364, and is the
wavelength in nanometers. The optical densities defined by Equation 1,
before any shifts, peak at 528.2 nm. We emphasize that this
photopigment spectrum was derived strictly for this analysis and is
useful only in the range of measured wavelengths (400-700 nm). In a
forthcoming publication we will use the spectral sensitivity data
reported here to derive a new photopigment density spectrum and
template. Although very similar to spectra measured by suction
electrode recordings, those obtained from psychophysics are slightly
steeper at longer wavelengths, probably because the suction electrode
data are measured transversely through the photoreceptor outer segment
rather than axially along it as in normal vision. Axial beams are
subject to waveguiding by the structure of the photoreceptor (for
further discussion, see .
In deriving this template and analyzing the spectral sensitivity data,
we made the simplifying assumption that the family of red, green, and
red-green hybrid photopigment spectra are invariant in shape when
plotted as a function of log( ) (Mansfield and Levine, 1985 ;
Stockman and Sharpe, MacNichol, 1986 ; Lamb, 1995 ). This simplification provides a
straightforward means of analyzing the spectral sensitivity data,
because the max of each photopigment can be estimated
from a simple shift of the polynomial defined by Equation 1 (see also
Baylor et al., 1987 ). A polynomial was used because we required a
simple, continuous function that could be shifted along the log
wavelength scale.
The primary fit of the photopigment template (Eq. 1) to the data was
performed in the single fitting procedure defined by Equations 2 and
3a:
|
(2)
|
|
(3a)
|
In Equation 2, the template,
POD(x), is shifted by x
log nanometers along the log wavelength scale and adjusted to a peak photopigment optical density of 0.5 to give the spectral sensitivity at
the retinal level, Sretina(x). In
Equation 3a, the spectral sensitivity at the retina,
Sretina(x), then is corrected to the cornea, Scornea(x), by restoring the
filtering effects of the lens pigment,
alensOD(x), and macular pigment,
bmacOD(x), two pigments that lie
between the cornea and the photoreceptor. We assumed the lens pigment
density spectrum [lensOD(x)] of van Norren and
Vos (1974) , slightly modified by Stockman et al. (1993a) , and a macular
pigment density spectrum [macOD(x)] based on
the Vos (1972) estimate. Vertical shifts
(cn) were estimated for each of the
n runs performed by each subject. Separate shifts for each run were required, because the short and long wavelength data sometimes
were measured during separate runs. The lens density multiplier
(a), the macular density multiplier (b), the
template shift ( x), and vertical shifts
(cn) are all best-fitting values determined by the fit of the model defined by Equations 1, 2, and 3a to
each set of data. The fit was performed with the Marquardt-Levenberg algorithm implemented in SigmaPlot (Jandel Scientific). In preliminary trials we also attempted to optimize the peak photopigment optical density (rather than assuming the fixed value of 0.5 in Eq. 2), but we
found that it was too poorly constrained. We therefore fixed it at 0.5 for each observer (see .
In the primary analysis defined by Equations 1, 2, and 3a, which we
refer to as the "full spectrum" fit, we fit the model at all
measured wavelengths. In the secondary analysis, which we refer to as
the "partial spectrum" fit, we performed the fit only for
measurements made at wavelengths 520 nm. This simplifies the fitting
procedure, because macular pigment plays little role, and the lens is
relatively transparent (having an average optical density of only 0.10 log unit at 520 nm that declines with wavelength). Equation 3a was
replaced by Equation 3b:
|
(3b)
|
The lens and macular densities were fixed at the mean population
densities obtained in the full spectrum fit. Thus,
lensOD(x) is 1.48 at 400 nm and
macOD(x) is 0.37 at peak (see Table 5, and
below). The average data for each subject were used for this fit so
that there is only a single vertical shift (c). The template shift ( x) and vertical shift (c) are
best-fitting values determined by the fit of the model defined by
Equations 1, 2, and 3b to the mean data ( 520 nm) for each subject.
The partial spectrum fit served, in part, as a control for the full
spectrum fit and in particular for the reliance (Eq. 3a) on
best-fitting macular and lens densities, which could, in principle,
distort the max estimates. Nonetheless, small
differences between the max estimates obtained by the
two methods should be expected, because the lens density assumed for the partial fit is the population mean density rather than
the optimized individual density. We estimate that increasing and
decreasing the lens density in Equation 3b by, for example, ±25%
results in changes in max of approximately ± 0.5 nm. Given that small differences are expected between the two
estimates, the agreement between the two is extremely good (see Tables
3-5; Figs. 7-9).
We note that fits using just the long wavelength portion of the
spectral sensitivity functions (Stockman and Sharpe, Baylor et al., 1987 ), in which
individual differences in lens and photopigment density differences
play little or no little role, are impracticable for our data. The
problem is that we do not know precisely the absolute differences in
sensitivity between the functions (i.e., their vertical positions
relative to each other). We cannot tell from just the long wavelength
part of the spectrum whether the difference between two functions is
attributable to a difference in absolute sensitivity (vertical shift)
or a difference in max (horizontal shift). We overcame
this problem by fitting a photopigment template (Eq. 1) that includes,
for both the partial spectrum and full spectrum fits, the peak of the
photopigment curve as well as its long wavelength slope. Such fits
allow us to determine both the vertical and the horizontal shifts together.
Below (see Tables 3-5), we use standard formats to define the results
of the two fits. We tabulate (1) the position of the fitted
photopigment template as its max in nanometers after the best-fitting shift ( x), (2) the best-fitting lens density
as the density at 400 nm, and (3) the macular density as the peak density of the pigment (at 460 nm). The SEs associated with each fit
parameter also are given, along with the root mean-squared (rms) errors
of the fits for each subject. The vertical shifts (c and
cn), because they are of little interest
in the context of this paper, are not tabulated individually. The mean
value of cn is 8.17 log quanta · sec 1 · degree 2 ( 8.10 for
protanopes and 8.22 for deuteranopes) with a SE of 0.08, whereas the
mean value of c is 8.17 log quanta · sec 1 · degree 2 ( 8.14 for
protanopes and 8.19 for deuteranopes) with a SE of 0.06. These values
indicate the mean peak flicker photometric sensitivities on the 420 nm
background field.
It is important to recognize that the spectral shifts ( x)
and the photopigment template
[POD(x)] are calculated in log
nanometers. Thus, the spectral shift in nanometers increases
with wavelength. For example, a shift of 2.49 nm (full spectrum
analysis; see Fig. 7B) or 2.69 nm (partial spectrum
analysis; see Fig. 8B) between the R(S180) and
R(A180) photopigments at their max becomes a shift of
3.08 nm and 3.33 nm, respectively, at 690 nm.
Systematic errors in both fits would be expected if different red-green
photopigments are not shape-invariant when plotted against
log10( ) or if the peak photopigment optical density
varies with genotype. Such errors would cause small shifts in the
max estimates between genotypes but would have little
effect on estimates within genotypes. Individual differences in
photopigment optical density within a genotype will, of course,
increase the variability of the max estimates within
that group. As noted above, small errors in the secondary fit should be
expected because of individual differences in lens pigment density.
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RESULTS |
Screening of dichromat subjects
Ninety-four dichromat males were recruited for this study. To
qualify, they needed to produce a Rayleigh match by merely adjusting the intensity of the yellow light, regardless of the red/green ratio
(Rayleigh, 1881 ). This is consistent with light absorption in this
region of the spectrum being mediated by a single type of
photoreceptor. To minimize confounding effects caused by age-related yellowing of the lens (Ruddock, 1965 ), we limited enrollment to young
adults (average age, 28 years old; range 16-45). If we assume 25%
efficient recruitment of subjects and a frequency of dichromacy among
European males of ~2% (Post, 1962 ), then we calculate that this
study required a base population of 120,000 people.
Analysis of visual pigment gene structure
Dichromacy can arise from either intragenic or intergenic
recombination within the tandem array of visual pigment genes (see Fig.
1) (Nathans et al., 1986b ; Deeb et al., 1992 ). In the simplest cases
the product of recombination contains either a single red pigment gene
as a result of intergenic recombination (producing deuteranopia, the
loss of green cone sensitivity; abbreviated here
G R+), or a single 5'red-3'green
hybrid gene as a result of intragenic recombination (producing
protanopia, the loss of red cone sensitivity; abbreviated here
G+R ). We will refer to subjects
who carry such an arrangement as "single-gene dichromats." As
described more fully below, the heterogeneity in 5'red-3'green
crossover points results in a variety of green-like pigments in
G+R dichromats, some of which
differ from the green pigments of normal trichromats. In a few more
complex cases the sequences suggest multiple recombination events. The
location of the 5' end of the red pigment gene at the edge of the
visual pigment gene array precludes the production of the reciprocal
hybrid i.e., a 5'green-3'red gene in an X chromosome that carries
only a single gene. 5'green-3'red hybrid genes are found in place of,
or in addition to, the normal green pigment gene(s) in
G'R+ subjects (Nathans et al., 1986b ; Deeb et al.,
1992 ).
The red and green visual pigment genes each consist of six coding
exons. Coding region sequence differences between these genes are
confined to exons 2-5, which encode the seven membrane-embedded -helices that together form the chromophore binding pocket. The present study confirms earlier observations that most intragenic recombination events between red and green pigment genes occur within
intron sequences, presumably because of the ~10-fold greater size of
the introns as compared with the exons and the paradoxically greater
DNA sequence similarity of the red and green pigment gene introns as
compared with the exons (Shyue et al., 1994 ). Thus, in general,
red-green hybrid genes contain some number of contiguous exons from one
end of a red pigment gene joined to the remaining exons from the other
end of a green pigment gene. In this paper, each hybrid pigment or the
gene that encodes it is referred to by an abbreviation that reflects
the origin of its exons and the identity of the polymorphic residue
(alanine or serine) at position 180 in the third exon. For example,
R4G5(A180) is a hybrid pigment encoded by a gene in which exons 1-4
are derived from a red pigment gene, exons 5 and 6 are derived from a
green pigment gene, and position 180 is occupied by alanine. Red
pigment genes are designated R(A180) or R(S180) to indicate the
presence of alanine or serine, respectively, at position 180. Several
of the pigment gene sequences reported here reveal a green pigment gene
exon 2 embedded within a red pigment gene or a 5'red-3'green hybrid
gene. In these cases the identity of the second exon is indicated in
parentheses; for example R(G2;A180) represents a gene in which exons 1 and 3-6 are derived from a red pigment gene, exon 2 is derived from a green pigment gene, and position 180 is occupied by alanine. The fact
that sequence differences between red and green pigment genes are
confined to exons 2-5 implies that a R1G2 hybrid gene encodes a de
facto green pigment.
Genomic DNA from each subject was analyzed first by Southern blot
hybridization with a cDNA probe from exons 1 and 2 to determine the
number of X chromosome visual pigment genes (see Fig. 1, Table 1). As shown in Figure 1C,
this probe reveals two fragments from the red pigment gene and two from
the green pigment gene that differ as a result of sequence variation in
the first intron and in 5' flanking DNA. The 5' hybridizing fragment
from the red pigment gene, designated Br, is present
as a single copy in all trichromat and dichromat X chromosomes (Nathans
et al., 1986a ,b ). Intergenic or intragenic recombination events that
reduce the array to a single gene result in the loss of fragment
Bg and the loss of either Cr or
Cg, depending on the exact location of the point of
crossover.
As expected from previous studies (Nathans et al., 1986b ; Deeb et al.,
1992 ), multiple genotypes were found for both
G+R subjects and
G R+ subjects. In all, 41 of 94 dichromats (44%) were found to carry a single X-linked visual pigment
gene. From these single-gene dichromats, DNA encompassing exons 2-5
was amplified and sequenced by using primers flanking each exon. In
each of the 41 cases, a unique sequence was obtained for the four
exons, consistent with the assignment of a single gene by Southern
blotting. Exons 2-5 also were amplified and sequenced from four
dichromats for which the Southern blot patterns predicted two or more
genes (subject numbers 42-45 in Table
2). Three of the four (HS2288, HS2293, and HS2312) show a superposition of different DNA sequences; the fourth
(HS2303) carries two or more genes with identical coding region
sequences.
A comparison of the deduced amino acid sequences from the 45 dichromats
shows variations at 19 positions, most of which can be associated with
either the normal green or the normal red pigment (Table 2). In each
case the variable position encodes one of two possible amino acids, and
most of these are located within the predicted transmembrane
-helices (Fig. 3). Previous work has
implicated amino acid substitutions at three of these positions 180, 277, and 285 as major determinants of the difference in spectral sensitivity between red and green pigments (Neitz et al., 1991 ; Merbs
and Nathans, 1992a ,b , 1993 ; Asenjo et al., 1994 ). Amino acid
substitutions at several other locations play a lesser role in spectral
tuning (Merbs and Nathans, 1992b ; Asenjo et al., 1994 ).

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Figure 3.
Schematic diagram of the human red and green
pigments in the membrane. The N terminus
(N) faces the extracellular space, and the
C terminus (C) faces the cytosol. Each
filled circle represents a position that differs between
red and green pigments in the set of sequences studied here; these are
positions 65, 111, 116, 153, 171, 174, 178, 180, 230, 233, 236, 249,
274, 275, 277, 279, 285, 298, and 309. The locations of
lysine312 (K312), the site of
covalent attachment of 11-cis retinal, and the
polymorphic serine/alanine at position 180 (A180/S180)
are indicated. The five intron positions are indicated by
vertical arrows.
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In accordance with the observations of Winderickx et al. (1993) on
visual pigment gene arrays in normal trichromats, we find that exon 3 is more variable than exons 2, 4, or 5. Except for position 180, the
highly polymorphic nature of the amino acids within exon 3 makes it
impossible to discern whether any particular exon 3 is derived from a
red or a green pigment gene, as can be seen by comparing the exon 3 sequences listed in Table 2. A quantitative representation of this
variability among red pigment genes is shown in Figure
4, in which the number and frequency of
distinct amino acid sequences is plotted for each exon for those 28 G R+ dichromats who carry a
single red pigment gene. This group of subjects is presumed to carry a
representative sample of normal red pigment genes, having lost their
green pigment genes by intergenic recombination.

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Figure 4.
Distribution by exon of amino acid sequence
variation in 28 red pigment genes (subjects 1-28 in Table 1). This
tabulation includes all subjects with genotypes R(A180), R(S180),
R(G2;A180), or R(G2;S180). Each bar in the histogram
represents a distinct amino acid sequence for a given exon, and these
are plotted on the horizontal axis for exons 2-5. The vertical axis
shows the frequency of each type of sequence. Exon 3 shows greater
polymorphism than exons 2, 4, or 5 do.
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Current estimates suggest that among human red pigment genes ~62%
have serine and 38% have alanine at position 180, whereas among green
pigment genes ~9% have serine and 91% have alanine at position 180 (Winderickx et al., 1993 ). Our finding, among 28 G R+ single-gene dichromats, of
21 R(S180) or R(G2;S180) genes and 7 R(A180) or R(G2;A180) genes is
approximately consistent with these published allele frequencies for
the red pigment gene. This distribution of the alanine/serine
polymorphism is relevant to the assignment of the origin of exon 3 among red-green hybrid genes in which crossover occurred between exons
2 and 3 or between exons 3 and 4. Among red-green hybrid genes that
carry serine at position 180, exon 3 (within which codon 180 resides)
is more likely to derive from a red pigment gene, whereas among
red-green hybrid genes that carry an alanine at position 180, exon 3 may have originated from either a green or a red pigment gene. Among subjects with R2G3 or R3G4 genotypes, we will, as a convention, refer
to those genes that have serine at position 180 as R3G4 hybrids and
refer to those genes that have alanine at position 180 as R2G3 hybrids.
Rayleigh matches
A comparison of the slopes of the regression lines fit to the
Rayleigh matches for 29 single-gene dichromats tested with a König-Helmholtz colorimeter is shown in Figure
5A for protanopes and Figure
5B for deuteranopes. The values, which also are tabulated in
Table 4, below, have not been corrected for absorption by the lens or
macular pigment; the latter should be minimal at the wavelengths used
(>546 nm; Wyszecki and Stiles, 1982 ). A progressive increase in the
slopes of the regression lines fit to the Rayleigh matches, reflecting
an increase in the ratio of red to green light required to match the
yellow standard, is seen for subjects whose X-linked pigment contains
progressively more green pigment-derived sequences. This is apparent in
comparing the red pigments R(A180) and R(S180) and the 5'red-3'green
hybrid pigments R4G5, R3G4, R2G3, and R1G2. The effect of alanine
versus serine at position 180 is reflected in the differences in the
slopes of the R(S180) and the R(A180) subjects. The former have a mean
slope of 0.396, and the latter have a mean slope of 0.459, with some
overlap in the distribution of individual data points. No significant
difference is apparent between the mean slopes of the three R1G2(A180)
subjects and the two R2G3(A180) subjects, nor are there significant
differences between the slopes obtained for those single-gene
dichromats who carry a red pigment gene versus those two subjects who
carry a red pigment gene in which the second exon has been replaced by a second exon derived from a green pigment gene [i.e., R(G2;A180) and
R(G2;S180)]. These data suggest that sequence differences in exon 2 play little or no role in determining the spectral differences among
red and green pigments. In general, however, the Rayleigh matches
provide limited information regarding spectral sensitivity because only
three wavelengths are sampled.

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Figure 5.
Slopes of the regression lines fit to the Rayleigh
matches obtained with a König-Helmholtz colorimeter for 29 single-gene dichromats. Data from protanopes are shown in A,
and data from deuteranopes are shown in B. The green,
yellow, and red primaries for this instrument were 546, 590, and 674 nm, respectively. The data have not been corrected for preretinal
absorption. An increase in slope is apparent for subjects with pigments
predicted to absorb at shorter wavelength. The mean values for the
slopes of R(A180) and R(G2;A180) subjects are 0.452 ± 0.30, and
for R(S180) subjects are 0.393 ± 0.012, a significant difference.
The mean values for the slopes of R1G2(A180) and R2G3(A180) subjects,
0.801 ± 0.056 and 0.770 ± 0.05, respectively, are not
significantly different (see Table 5).
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Spectral sensitivity measurements
Foveal spectral sensitivities were determined in 40 subjects (37 single-gene and 3 multiple-gene dichromats) by heterochromatic flicker
photometry. As noted in Materials and Methods, a reference light of 560 nm was alternated at a rate of 16 or 25 Hz with a superimposed test
light, the wavelength of which was varied in 5 nm steps from 400 to 700 nm. Subjects found the radiance of the test light that eliminated or
"nulled" the perception of flicker produced by the alternation of
the two lights. Because the blue cones are desensitized by the
background (and in any case make little contribution to flicker
photometry under most conditions; Eisner and MacLeod, 1980 ;
Stockman et al., 1991 ) and the rods are saturated, the nulled test and
reference lights produce an equivalent level of activation of the
remaining single class of red, green, or red-green hybrid cone in each
single-gene dichromat. The radiance of the test light required to null
the reference light as a function of wavelength is therefore an
estimate of the spectral sensitivity of each subject's single longer
wavelength cone type.
Figure 6 shows representative examples of
the heterochromatic flicker data (symbols) for four subjects. The data
sets for subjects HS2313, HS2188, and HS2237 are examples of the best, intermediate, and worst fits, respectively. The data set for subject HS2243 is an example of an intermediate fit, but with limited data. We
have similarly limited data for 5 of the 40 subjects.

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Figure 6.
Representative examples of cone spectral
sensitivity data (filled symbols) for four
single-gene dichromats: HS2313 (top), HS2188
(upper middle), HS2237 (lower middle),
and HS2243 (bottom), together with the fits of the
visual pigment template (continuous lines). Data are
from several single runs. The data sets for HS2313, HS2188, and HS2237
are examples of the best, intermediate, and worst fits, respectively,
of the visual pigment templates to the data. The data set for subject
HS2243 is an example of a subject for whom we have limited data. For
clarity, the data sets have been displaced vertically.
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We analyzed the spectral sensitivity measurements for each observer to
estimate the wavelength of maximum sensitivity
( max) of his underlying longer wavelength cone
photopigment by using either the full range of measured wavelengths
(400-700 nm), the "full spectrum" analysis (see Eqs. 1, 2, and 3a,
below), or wavelengths 520 nm, the so-called "partial spectrum"
analysis (see Eqs. 1, 2, and 3b, below).
In the full spectrum fit we determined the best-fitting macular and
lens pigment densities as well as the spectral position of the
underlying pigment template. The results are tabulated in Table
3, along with each subject's age and the
rms error of the fit. Also tabulated are the SEs for each fitted
parameter. A compilation of the max values and the SEs
is shown in graphic form in Figure 7 for
each protanope (Fig. 7A) and deuteranope (Fig.
7B). The full spectrum fits to the data for subjects HS2313, HS2188, HS2237, and HS2243 are shown by the continuous lines in Figure
6.
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Table 3.
Best-fitting photopigment max values and
macular and lens densities according to the full spectrum analysis
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Figure 7.
max values for red, green, or
red-green hybrid pigments for individual dichromats grouped by
genotypic class. The values shown here are from the full spectrum
analysis with best-fitting lens and macular pigment corrections (see
Table 3). The error bars indicate the SEs of the
max estimates. A, Protanopes: R1G2(A180),
filled circles; R1G2(A180)+G(A180), filled
square; R2G3(A180), filled triangles;
R2G3(A180)+G(A180), filled inverted triangles;
R3G4(S180), filled diamonds; R4G5(A180) gene,
filled hexagon; and R4G5(S180), open
square. B, Deuteranopes: R(A180), filled
squares; R(G2;A180), open square; R(S180),
filled circles; and R(G2;S180), open
circle. The vertical dashed lines represent the
mean max estimates for the R(A180) and R(G2;A180)
observers (left line, 557.68 nm) and R(S180) and
R(G2;S180) observers (right line, 560.17 nm). The
spectral difference between the two means is 2.49 nm.
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In the partial spectrum fit we fixed the macular and lens pigment
densities at their mean best-fitting values and determined only the
spectral position of the underlying pigment template. The results are
tabulated in Table 4, and a compilation
of the max values and the SEs is shown in Figure
8. The partial spectrum fit also acts as
a control for the full spectrum fit. Any distortion of the full
spectrum max estimate caused by optimizing the lens and
macular pigment densities should result in clear differences between
the full spectrum and partial spectrum. These differences will be in
addition to the small discrepancies that arise because mean rather than
optimal lens and macular densities are assumed in the partial spectrum
fit (see Materials and Methods).
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Table 4.
Best-fitting photopigment max values
according to the partial spectrum ( 520 nm) analysis, and slopes of
the regression lines fit to Rayleigh matches
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Figure 8.
max values for red, green, or
red-green hybrid pigments for individual dichromats grouped by
genotypic class. The values shown here are from the partial spectrum
( 520 nm) analysis with mean lens pigment corrections (see Table 4).
The error bars indicate SEs of the max estimates.
A, Protanopes. B, Deuteranopes. The
vertical position of each subject's data point is the same as in
Figure 7. Symbols are as in Figure 7. The
vertical dashed lines represent the mean
max estimates for R(A180) and R(G2;A180) observers
(left line, 557.53 nm) and R(S180) and R(G2;S180)
observers (right line, 560.22 nm). The spectral
difference between the two means is 2.69 nm.
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Figure 9 presents a comparison of the
max estimates obtained by the two methods. The estimates
for the protanopes lie close to a straight line of unit slope
(continuous line), which indicates good agreement between the two
methods. The disagreements are <0.59 nm, with a mean of 0.06 nm (and
a mean of 0.29 nm for the absolute differences). The estimates for
deuteranopes fall along a slightly steeper line, with a best-fitting
slope (Fig. 9B, dashed line) of 1.12, which suggests that
the full spectrum fit, relative to the partial spectrum fit, slightly
underestimates the max of longer wavelength red cone
photopigments but overestimates that of shorter wavelength ones. In
this case the discrepancies are <0.80 nm, with a mean of 0.00 nm (and
a mean of 0.37 nm for the absolute differences).

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Figure 9.
max values obtained from the full
spectrum analysis plotted against those obtained from the partial
spectrum ( 520 nm) analysis. The continuous diagonal
lines (with slopes of 1) indicate perfect agreement between the
two analyses. The regression line for protanopes
(A) has a slope of 1.00 and is indistinguishable
from the diagonal line, whereas that for deuteranopes
(B) has a slope of 1.12, as shown by the
dashed line. Symbols are as in Figures 9
and 10. Perfect agreement should not be expected between the two
analyses because mean, rather than individual, macular and lens
densities are used in the partial spectrum, but not full spectrum,
analysis.
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We consider first the individual deuteranopic spectral sensitivities
(see Figs. 7B, 8B, 9B, Tables
3, 4). The estimated max values for four R(A180)
subjects span a range of 2 nm, whereas those for 18 R(S180) subjects
span a range of 4 nm with a partial overlap between the two
populations. The max values of these various red
pigments range from 556.8 to 562.1 nm (full spectrum analysis; Table 3)
or from 556.2 to 562.7 (partial spectrum analysis; Table 4). Among the
10 R(S180) subjects with identical amino acid sequences (HS2173,
HS2176, etc; see Table 2), the max values average
560.6 ± 0.4 with a range of 558.0 to 562.1 nm (full spectrum analysis; Table 3) and 560.4 ± 0.4 nm with a range of 557.7 to 562.7 nm (partial spectrum analysis; Table 4). Because this
subject-to-subject variation occurs within the context of identical
cone pigment sequences, it provides a measure of the precision with
which these data and the analyses can be used to define the cone
spectral sensitivity associated with a given pigment type. The
max values of the two pigments that carry a green exon 2 embedded within an otherwise red pigment gene [R(G2;A180) and
R(G2;S180)] are located on the short-wave limb of the corresponding
R(A180) or R(S180) distributions, respectively. These data suggest that
in this context a change in exon 2 from R2 to G2 shifts the
max to slightly shorter wavelengths, but in terms of the
distributions the effect is not significant. If we include the two
types of R(G2) pigments together with their corresponding red pigments, then the means of the max values for the A180 and S180
red pigments have a separation of 2.49 nm (full spectrum analysis;
Table 3) and 2.69 nm (partial spectrum analysis; Table 4). The
variation in max among the 17 R(S180) subjects does not
correlate in any simple way with the other polymorphic amino acids in
exon 3.
The max values for 13 single-gene protanopes with
5'red-3'green hybrid pigments and three with two or more green or
green-like pigments [i.e., R1G2+G(A180) and R2G3+G(A180)] are within
the interval 525.6-535.5 nm (full spectrum analysis; Fig.
7A, Table 3) or 525.5-535.4 nm (partial spectrum analysis;
Fig. 8A, Table 4). These data confirm the major role
of exon 5 sequence differences in determining the spectral separation
between red and green pigments (Neitz et al., 1991 ; Merbs and Nathans,
1992b , 1993 ; Asenjo et al., 1994 ). Although the number of individuals
with pigments of each type is small and there is variation of up to 3.5 nm in max values within a genotype, the spectral
sensitivity measurements show a clear trend toward longer values of
max for those pigments with a greater number of red
pigment exons. In particular, the individual data indicate that there
is, on average, a ~1 nm spectral shift to longer wavelengths (range,
0.5 to 2.5 nm) associated with a change in exon 2 from green to red
pigment sequences, a value similar to that described above for the red
pigment and not statistically significant. This value for the average
spectral shift associated with differences in exon 2 is influenced
significantly by one subject (HS2196) whose max (525.6 nm) is unusually short; without HS2196, the mean shift is <1 nm. For
exon 4 the change from green to red pigment sequences is associated
with, on average, a ~2.8 nm spectral shift (range, 0.5 to 6 nm) to
longer wavelengths. Finally, these data suggest that polymorphic amino
acid sequence variations in exon 3 are associated with an average
spectral shift of ~3.3 nm, with a range from 0.5 to 7 nm.
To examine the effect of serine or alanine at position 180 among
5'red-3'green hybrid pigments, we can make a comparison between subjects who have either R2G3 or R3G4 genotypes. These genotypes can be
considered together because, as noted above, except for position 180, the polymorphic nature of the other amino acids within exon 3 makes it
impossible to discern whether it is derived from a red or a green
pigment gene. A comparison between the five subjects with a R3G4(S180)
pigment and the five subjects with R2G3(A180) or R2G3+G(A180) pigments
shows a mean red shift of 2.5 nm (full spectrum analysis; Table 3) or
2.3 nm (partial spectrum analysis; Table 4) caused by the presence of
serine at position 180. By contrast, the single subject with a
R4G5(S180) pigment has a max that is 1.5 nm blue-shifted
relative to the single subject with a R4G5(A180) pigment. Given the
observations just noted with larger numbers of subjects that indicate a
red-shifting effect of serine at position 180 and the several nanometer
variability in max values among subjects with identical
genotypes, we think that experimental variability and/or an unusual
photopigment optical density may account for the unexpected
relationship between this single pair of max values.
As well as individual data, we can consider mean spectral sensitivity
data. Figure 10 shows data averaged
across (1) five observers with a single R(A180) (n = 4)
or R(A180;G2) gene (n = 1) (white squares); (2) 15 observers with a single R(G2;S180)
(n = 1) or R(S180) (n = 14) gene
(black squares); and (3) nine observers with a single
R1G2 (n = 3) or R2G3 (n = 3) gene or
with multiple R1G2+G (n = 1) or R2G3+G
(n = 2) genes (gray circles).
These mean analyses, with the exception of (1), include only subjects
who made measurements throughout the spectrum. We have averaged
together data from subjects whose genes differ only in their second
exon (green vs red), because the substitution of a green for a red exon
2 does not alter spectral sensitivity significantly (Table 5). Table 5 lists the results of the full
spectrum and partial spectrum fits and the Rayleigh matches averaged
across genotypes.

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Figure 10.
Averaged spectral sensitivity measurements for
green, red(A180), and red(S180) pigments. Shown are mean data for nine
observers with a single R1G2 (n = 3) or a single
R2G3 (n = 3) gene or with multiple R1G2+G
(n = 1) or R2G3+G (n = 2) genes
(gray circles), five observers with a single
R(G2;A180) (n = 1) or R(A180)
(n = 4) gene (white squares), and 15 observers with a single R(G2;S180) (n = 1) or a
single R(S180) (n = 14) gene (black
squares). Three of the five R(A180) group made measurements
only at wavelengths >470 nm, so the mean data are restricted to that
region. The other means include data only from subjects who made
measurements throughout the spectrum. Error bars indicate SE. The
continuous lines fit to each set of data 520 nm are
fits of the partial spectrum model (Eqs. 1, 2, and 3b) to the mean
data. See Materials and Methods for details.
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Figure 11 shows the mean spectral
sensitivity data for protanopes with red-green hybrid photopigments.
The gray circles are the same as in Figure 10; that is, they are the
averages of data from the nine observers with single or multiple R1G2,
R2G3, or green photopigment genes. The black circles denote the
averages of data from the four observers with a single R3G4(S180) gene, whereas the white inverted triangles and white triangles are the individual data for the single observers with a R4G5(A180) and a
R4G5(S180) gene, respectively.

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Figure 11.
Averaged spectral sensitivity measurements for
red-green hybrid pigments. Shown are mean data for nine observers with
R1G2 or R2G3 genes [a single R1G2 (n = 3) or a
single R2G3 (n = 3) gene or multiple R1G2+G
(n = 1) or R2G3+G (n = 2)
genes] (gray circles), for four observers with a
single R3G4(S180) gene (black squares), for one observer
with a single R4G5(A180) gene (white inverted triangle),
and for one observer with a single R4G5(S180) gene (white
triangle). The mean data are only from subjects who made
measurements throughout the spectrum. Of the protanopes, only one
R3G4(S180) observer did not make complete measurements. Error bars
indicate SE. The continuous lines fit to each set of
data 520 nm are fits of the partial spectrum model to the mean or
individual data. See Results for details.
|
|
The continuous lines fit to each set of data in Figures 10 and 11 are
fits of the partial spectrum model (Eqs. 1, 2, and 3b) to the mean
data. The max values of the fitted templates and the SEs
of the fit are 557.5 ± 0.4 nm [R(A180)]; 560.4 ± 0.3 nm [R(S180)]; 528.56 ± 0.2 nm [R1G2/R2G3]; and 531.5 ± 0.3 nm [R3G4(S180)]. For the individual R4G5(A180) and R4G5(S180) data,
the fits are as also given in Tables 4 and 5: 535.4 ± 0.4 nm
[R4G5(A180)] and 533.9 ± 0.3 nm [R4G5(S180)]. The fits to the
mean data agree well with the averages of the individual fits (see
Table 5), although the R(S180) versus R(A180) difference of 2.9 nm is
slightly larger than the differences estimated from the individual data (2.7 and 2.5 nm for the partial and full spectrum fits, respectively).
 |
DISCUSSION |
Genotype and phenotype among single-gene dichromats
By correlating the X-linked visual pigment sequences and
color vision phenotypes of single-gene dichromats, we have
characterized the spectral sensitivities in vivo of cones
containing the normal human red and green pigments, as well as a series
of 5'red-3'green hybrid pigments. We have determined psychophysically
the spectral sensitivities of 37 single-gene dichromats and three
dichromats who carry more than one X-linked visual pigment gene. Other
investigators have reported DNA sequences and spectral sensitivities by
using electroretinographic methods for small numbers of dichromats with one or more visual pigment genes (Neitz et al., 1995b ), and our results
are in approximate agreement with their data. The study of single-gene
dichromats greatly simplifies the correlation of genotype and
phenotype, and this approach should lead eventually to a comprehensive
catalog of the spectral sensitivities of the various red, green, and
5'red-3'green hybrid pigments. The most significant limitation of using
single-gene dichromats is that they do not carry 5'green-3' red hybrid
genes, which therefore can be studied only in G'R+
anomalous trichromats.
Amino acid substitutions and spectral shifts
The psychophysical data reported here indicate that 5'red-3'green
hybrid genes encode a range of pigments with altered spectral sensitivities and that in every case examined the spectral sensitivity of the hybrid is between those of the normal red and green pigments. The data further indicate that the spectral sensitivity of the hybrid
depends on the position of the crossover and on the identity of other
polymorphic amino acids, principally alanine or serine at position 180. For each exon the set of amino acids normally associated with the red
or green pigments produces, respectively, spectral shifts to longer or
shorter wavelengths, thus producing a monotonic relationship between
the max and the fraction of the hybrid pigment derived
from the red and green parental pigments.
The primary determinants of the spectral shift are located in exon 5, as seen by the clustering of the absorption maxima of all 5'red-3'green
hybrids within 10 nm of the maxima of the normal green pigments (Tables
3-5; Figs. 7, 8) (Merbs and Nathans, 1992b ; Asenjo et al., 1994 ). A
comparison of the spectral sensitivities of R(A180) and R(S180) with
those of R4G5(A180) and R4G5(S180) indicates that red/green sequence
differences in exon 5 result in a spectral shift of ~25 nm (see Figs.
7-10). The spectral sensitivity data further suggest that exon 2 contributes on average ~1 nm (range, 0.5 to 2.5 nm), whereas exon 3 contributes on average ~3.3 nm (range, 0.5 to 7 nm), exon 4 contributes on average ~2.8 nm (range, 0.5 to 6 nm), and exon 5 contributes on average ~24.9 nm (range, 22.2 to 27.6 nm). These
results are in approximate agreement with results obtained from
recombinant human cone pigments produced in transfected cells and
studied in detergent solution (Merbs and Nathans, 1992b ; Asenjo et al.,
1994 ) and with inferences based on a comparison of primate visual
pigment gene sequences and cone spectral sensitivity curves (Neitz et
al., 1991 ; Ibbotson et al., 1992 ; Williams et al., 1992 ).
Over the past 6 years considerable attention has been paid to the
importance of the serine/alanine polymorphism at position 180 (Merbs
and Nathans, 1992a ,b ; Winderickx et al., 1992a ; Sanocki et al., 1993 ,
1994 ; Asenjo et al., 1994 ; Neitz et al., 1995b ). All of the reported
measurements have shown that serine-containing pigments are red-shifted
with respect to alanine-containing pigments, but the magnitude of the
shift has been controversial. Previous psychophysical and
electroretinographic studies aimed at measuring the spectral shift
produced by substitution at this position have been complicated by the
presence of additional genes and/or additional amino acid substitutions
within the same gene. On the basis of anomaloscope matches, Sanocki et
al. (1993 , 1994 ) estimated that the substitution of alanine by serine
in the red pigment or within 5'red-3'green hybrid pigments results in a
red shift of max by 4.3, 3.5, and 2.6-2.7 nm for
G R+ dichromats,
G+R dichromats, and normal
trichromats, respectively. Neitz and Jacobs (1990) estimated a red
shift of ~3 nm from Rayleigh match data obtained from 60 normal
trichromats. Red shift estimates of 5-7 nm were obtained from five
dichromats by electroretinography, but this interpretation was
complicated by additional amino acid differences between the pigments
(Neitz et al., 1995b ). In vitro measurements of recombinant
pigments by Merbs and Nathans (1992a ,b ) showed a red shift of 4.3-4.4
nm in the red pigment and in 5'red-3'green and 5'green-3'red hybrid
pigments. By contrast, Asenjo et al. (1994) found a range of red shifts
depending on the parental pigment: a 2 nm shift in a 5'red-3'green
hybrid and in the green pigment, a 4 nm shift in a 5'green-3'red
hybrid, and a 7 nm shift in the red pigment. We do not have an
explanation for the discrepancy between the 7 nm value reported by
Asenjo et al. and the smaller values reported by Merbs and Nathans and
obtained here. The spectral sensitivity curves reported here show a
mean separation of 2.5-2.9 nm, depending on which of two methods is
used to calculate the spectral sensitivity curve and whether individual
or mean data are used. These results are consistent with other
psychophysical measures of the variability of the red cone
max in the normal population (Webster and MacLeod, 1988 ;
Webster, 1992 ). The individual variation present in each genotypic
group emphasizes the importance of averaging data from large numbers of subjects.
Implications for models of dichromacy and
anomalous trichromacy
These results have significant implications for current theories
of dichromacy. Most importantly, they require a qualification of the
classical theory that all dichromats are merely missing one of the
normal pigments and retain the others unchanged (the reduction model;
Maxwell, 1860 ; König and Dieterici, 1886 ). Over one-half of the
dichromats analyzed in this study (53/94) carry and presumably express
more than one X-linked visual pigment gene. For
G R+ dichromats (deuteranopes)
these larger arrays consist of a normal red pigment gene and a
5'green-3'red hybrid gene that encodes a pigment with a spectral
sensitivity similar to that of the normal red pigment (Nathans et al.,
1986b ; Deeb et al., 1992 ). For
G+R dichromats (protanopes)
these larger arrays consist of a 5'red-3'green hybrid gene that encodes
a pigment with a spectral sensitivity similar to that of a green
pigment and one or more normal green pigment genes (Nathans et al.,
1986b ; Deeb et al., 1992 ). Among single-gene dichromats those with
G R+ dichromacy constitute a
true reduction type. By contrast,
G+R single-gene dichromats
possess any one of several green-like hybrid pigments, and in the
present study only 3 of 13 were found to possess a bona fide green
pigment (i.e., a pigment encoded by a R1G2(A180) hybrid gene). An
additional 3 of 13 possess a R2G3(A180) hybrid pigment, which has an
absorbance spectrum that is identical or nearly identical to that of a
normal green pigment. However, 7 of 13 G+R single-gene dichromats
reported here possess R3G4 or R4G5 hybrids, which would be predicted to
produce G+R' anomalous trichromacy if found in place
of a red pigment gene and in conjunction with one or more normal green
pigment genes. Thus, these subjects, who were found in this study to
constitute 19% of all G+R
dichromats, can be thought of as "anomalous protanopes."
The results described here are also relevant to contemporary theories
of anomalous trichromacy. Although we have only studied anomalous
pigments in dichromats, such pigments can, as noted above, be expressed
from more complex gene arrays and, when paired with a normal pigment,
produce anomalous trichromacy. Our finding of a diverse family of
hybrid pigments is not consistent with the theory that all anomalous
trichromats share a single anomalous pigment with a spectral
sensitivity at a position intermediate between the normal red and green
pigments (De Vries, 1948b ; MacLeod and Hayhoe, 1974 ; Hayhoe and
MacLeod, 1976 ), nor are the data consistent with the theory that there
is one anomalous pigment common to all G'R+
anomalous trichromats and another anomalous pigment common to all
G+R' anomalous trichromats (Rushton et al., 1973b ;
Pokorny et al., 1975 ; Pokorny and Smith, 1977 ; DeMarco et al., 1992 ).
Finally, the data do not support, in its most extreme form, the theory that there are no distinct anomalous pigments but instead clusters of
"normal" red and green pigments that differ in their peak
sensitivities, and that anomalous trichromats draw their pigments from
the same rather than different clusters (Alpern and Moeller, 1977 ;
Alpern and Wake, 1977 ). Although this theory fails to account for the existence of bona fide hybrid pigments, it explains the phenotypes of
that subset of anomalous trichromats in which the normal and anomalous
pigments are distinguished only by the polymorphic alanine versus
serine difference at position 180.
Any comprehensive model of anomalous trichromacy must account for the
fact that anomalous trichromats differ greatly in the location and
range of their Rayleigh matching points (for review, see Pokorny et
al., 1979 ; Mollon, 1997 ). The data presented here strongly support a
model of anomalous trichromacy in which any one of many green-like or
red-like anomalous pigments can be paired with either of two major
polymorphic versions of the more similar normal pigment (Merbs and
Nathans, 1992b ; Neitz et al., 1996 ). As the spectral sensitivities of
the normal or the anomalous pigments shift, the midpoint of the
Rayleigh match will shift, and as the separation between the
spectral sensitivities of the normal and anomalous pigments increases
or decreases, the better or poorer will be the subject's chromatic discrimination.
Implications for the derivation of human cone fundamentals
The traditional method of estimating the red and green cone
sensitivities is to use data obtained from
G R+ and
G+R dichromats. This approach
is only valid, however, if those dichromacies are truly reduced forms
of normal trichromacy in which one of the two normal X-linked pigments
is absent and the other is identical in its spectral properties to that
in the normal observer. As described above, the observations reported
here underscore several important caveats that affect the validity of
the reduction hypothesis. Moreover, the existence of polymorphism among
normal red or green pigment genes, most especially the serine/alanine
polymorphism at position 180, means that even true reduction dichromats
constitute a heterogeneous group. It follows that a single set of cone
fundamentals will describe accurately the color vision of only a subset
of normal trichromats and that in the construction of an average set of
fundamentals it is important that the ratio of polymorphic types within
the test population match that in the general population. Thus, the
most comprehensive approach to the construction of the cone
fundamentals would be to determine spectral sensitivity curves for a
large number of single-gene dichromats whose visual pigment gene
sequences reveal which of the various possible pigments they possess.
The averaged spectral sensitivity curves reported here for the R(A180),
R(S180), and the green-like R1G2(A180) and R2G3(A180) pigments
represent a first step toward this goal.
 |
FOOTNOTES |
Received March 24, 1998; revised Sept. 8, 1998; accepted Sept. 14, 1998.
This work was supported by The Deutsche Forschungsgemeinschaft (Bonn;
Grants SFB 430 Tp A6 and Sh23/5-1) and a Hermann und Lilly Schilling
Professor award (L.T.S.), the Howard Hughes Medical Institute (J.N.),
and the National Eye Institute (A.S.). We thank Drs. Donald MacLeod and
Edward Famiglietti and two anonymous reviewers for helpful comments on
this manuscript.
Correspondence should be addressed to Drs. Lindsay T. Sharpe, Andrew
Stockman, or Jeremy Nathans at the above addresses.
aAmong visual psychophysicists the three cone classes now most
often are referred to as long (L), middle (M), and short (S) wavelength-sensitive, according to the relative positions within the
visible spectrum to which they are most sensitive. Among molecular biologists an older usage, in which the cones are referred to as red
(R), green (G), and blue (B), is more prevalent. In this article, to be
consistent and to avoid confusion caused by converting between
terminologies, we adhere to the R, G, and B usage throughout. Hybrid
visual pigment genes are denoted as 5'red-3'green or 5'green-3'red, to
indicate which parental gene contributed sequences for the 5' end and
which contributed sequences for the 3' end of the hybrid gene.
 |
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