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Plant Physiol, January 2000, Vol. 122, pp. 147-156
Elementary Processes of Photoperception by Phytochrome A
for High-Irradiance Response of Hypocotyl Elongation
in Arabidopsis1,2
Tomoko
Shinomura,
Kenko
Uchida, and
Masaki
Furuya*
Hitachi Advanced Research Laboratory, Hatoyama, Saitama 350-0395,
Japan.
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ABSTRACT |
Elementary
processes of photoperception by phytochrome A (PhyA) for the
high-irradiance response (HIR) of hypocotyl elongation in Arabidopsis
were examined using a newly designed irradiator with LED. The effect of
continuous irradiation with far-red (FR) light could be replaced by
intermittent irradiation with FR light pulses if given at intervals of
3 min or less for 24 h. In this response, the Bunsen-Roscoe law of
reciprocity held in each FR light pulse. Therefore, we determined the
action spectrum for the response by intermittent irradiation using
phyB and phyAphyB double mutants. The
resultant action spectrum correlated well with the absorption spectrum
of PhyA in far-red-absorbing phytochrome (Pfr). Intermittent
irradiation with 550 to 667 nm of light alone had no significant effect
on the response. In contrast, intermittent irradiation with red light
immediately after each FR light pulse completely reversed the effect of
FR light in each cycle. The results indicate that neither red-absorbing
phytochrome synthesized in darkness nor photoconverted Pfr are
physiologically active, and that a short-lived signal is induced during
photoconversion from Pfr to red-absorbing phytochrome. The mode of
photoperception by PhyA for HIR is essentially different from that by
PhyA for very-low-fluence responses and phytochrome B for low-fluence responses.
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INTRODUCTION |
Light controls diverse processes of plant growth and development
(Mohr and Shropshire, 1983 ). Early physiological and photochemical studies indicated that light responses in photomorphogenesis are classified as a low- or high-energy reactions according to their energy
requirements (Mohr, 1962 ). Later, low-energy reactions induced by short
pulses of irradiation with relatively small doses of light, were
divided into low-fluence responses (LFRs, which early papers cited as
low-irradiance responses) and a very-low-fluence responses (VLFRs,
which early papers cited as very-low-irradiance responses) (Blaauw et
al., 1968 ; Mandoli and Briggs, 1981 ). The high-energy reaction, which
required a radiation with relatively high energy for a relatively
long period of time, was renamed a high-irradiance response (HIR)
(Briggs et al., 1984 ).
Phytochrome was first discovered as the photoreceptor for reversibility
by red (R) and far-red (FR) light (Butler et al., 1959 ), which was only
observed in LFRs. Recent studies using phytochrome-deficient mutants
demonstrated that phytochromes are photoreceptors for VLFR (Shinomura
et al., 1996 ) and HIR (Quail et al., 1995 ), although R/FR light
reversibility was not observed in either response.
HIR has been examined extensively in photoinhibition of stem elongation
and in anthocyanin production. Each of these responses requires
prolonged light irradiation treatment and depends on fluence rate
(Mohr, 1972 ; Smith et al., 1991 ). Action spectra for responses to the
prolonged irradiation were determined as a way to define the spectral
characteristics of putative photoreceptor(s), but they showed
complicated features; action maxima were found in the UV-B, UV-A, blue
light, R light, and FR light regions, and the action spectra varied
depending on the plant species, developmental stage, and growth
conditions before the spectral light treatment (Beggs et al., 1980 ;
Goto et al., 1993 ; Mancinelli, 1994 ). HIRs showing a peak in the FR
light region (Mohr, 1962 ) were called FR light-HIR, and the involvement
of phytochrome in the mediation of the FR light-HIR was speculated
based upon experimental results using prolonged dichromatic irradiation
with continuous R and FR light (Hartmann, 1966 ).
The discovery of type I and II phytochromes showing different stability
of far-red-absorbing phytochrome (Pfr) and molecular properties
(Furuya, 1989 ) and of the phytochrome multigene family (Sharrock and
Quail, 1989 ; Clack et al., 1994 ) opened new approaches to address which
member of the phytochrome family is responsible for which
phytochrome-mediated response(s) (Furuya, 1993 ). Among them,
phytochrome A (PhyA) and phytochrome B (PhyB) were assigned to mediate
HIR of photoinhibition of hypocotyl elongation in Arabidopsis (Quail et
al., 1995 ). The response induced by continuous R light was mediated
predominantly, if not exclusively, by PhyB (Nagatani et al., 1991 ; Reed
et al., 1993 ). Conversely, the responses induced by continuous FR light
were mediated predominantly by PhyA (Nagatani et al., 1993 ; Parks and
Quail, 1993 ; Whitelam et al., 1993 ). Given that VLFRs of seed
germination (Shinomura et al., 1994 , 1996 ) and Cab gene expression
(Hamazato et al., 1997 ) of Arabidopsis are induced by a brief light
irradiation mediated by PhyA, the question arises whether the
elementary process of photoperception by PhyA for induction of HIR is
the same as that for the induction of PhyA-mediated VLFR.
For several HIRs, including fern spore germination (Sugai et al., 1977 )
and hypocotyl elongation in dicots (Mohr, 1957 ; Hillman and Purves,
1966 ), the physiological effects of continuous R light could be
replaced by intermittent irradiation with R light pulses, and the
effect was reversed by pulses of FR light after each R light pulse. The
PhyB-mediated HIR of inhibition of hypocotyl elongation of Arabidopsis
was also examined by 4-h intermittent instead of continuous R
irradiation (McCormac et al., 1993 ). Using this light treatment, the
R/FR-light-reversible regulation and the validity of the Bunsen-Roscoe
law of reciprocity were shown at each pulse of R light (McCormac et
al., 1993 ). In the response obeying the Bunsen-Roscoe law of
reciprocity, the extent of the response is proportional to the photon
fluence, irrespective of whether that photon fluence is produced by
short irradiation with high photon fluence rate or longer irradiation
with low photon fluence rate (Schäfer et al., 1983 ). The validity
of the Bunsen-Roscoe law of reciprocity in PhyB-mediated HIR and LFR
means that just one photoreceptor contributes to a primary reaction of
each response as a rate limiting factor. Therefore, the elementary
process of the photoperception by PhyB for HIR (McCormac et al., 1993 )
appears to be consistent with that by PhyB for LFR (Shinomura et al., 1996 ).
In contrast, the PhyA-mediated inhibition of hypocotyl elongation in
Arabidopsis induced by continuous FR light was not induced by either FR
light pulses at 4-h intervals (McCormac et al., 1993 ) or FR light
pulses at 1-h intervals (Ahmad and Cashmore, 1997 ; Casal et al., 1998 ).
Therefore, it was not known whether the PhyA action for this response
is similar to PhyA-mediated VLFR, which is characterized by the
required range of photon fluence, the effective range of wavelength,
the validity of the Bunsen-Roscoe law of reciprocity, and the failure
of R/FR light reversibility.
To solve this problem, we designed and built a custom-made irradiation
system based on light-emitting diodes (LEDs) that allows us to control
the intermittent irradiation with R and FR light pulses for durations
of milliseconds to hours with any desired dark intervals. We describe
here elementary processes of photoperception by PhyA for inhibition
of hypocotyl elongation by cyclical pulse irradiation generated by
LEDs, the action spectrum by intermittent irradiation generated by the
Okazaki large spectrograph (Watanabe et al., 1982 ), and the opposite
effects of R and FR light pulses on the response. We discuss why
PhyA-mediated inhibition of hypocotyl elongation occurs under
continuous (and intermittent) irradiation with FR light but not with R
light (Nagatani et al., 1993 ; Parks and Quail, 1993 ; Whitelam et al.,
1993 ), despite both PhyA (Butler et al., 1959 ) and PhyB (Abe et al.,
1989 ) showing similar absorption spectra with peaks in the R light
region of the spectrum.
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MATERIALS AND METHODS |
Plant Growth Measurement
Wild-type seedlings of Arabidopsis Heynh. were of ecotype Ler
(Landsberg erecta); PhyA-deficient (phyA) mutant
seedlings were phyA-201 (ecotype Ler); PhyB-deficient
(phyB) mutant seedlings were phyB-1 (ecotype
Ler); and PhyA- and PhyB-deficient (phyAphyB) double-mutant
seedlings were produced from phyA-201 and phyB-1, unless otherwise indicated. Wild-type seedlings of ecotype Columbia and
phyB-9 mutant seedlings (ecotype Columbia) were also
examined when needed. For measurement of hypocotyl length,
approximately 60 seeds were planted on agar plates (Murashige and Skoog
medium diluted to one-tenth with 0.7% [w/v] agar) and kept at 4°C
for 3 d. Duplicate or triplicate plates were used for the
measurement of each data point. Plates were subsequently transferred to
23°C in the dark for 16 h, exposed to white light for 8 h
to induce seed germination, and then transferred to the dark for an
additional 40 h. These 2-d-old seedlings were irradiated with
pulses of LEDs or monochromatic light for appropriate periods, then
hypocotyls of the longest 30 seedlings were measured using a digimatic
caliper (CD-15C, Mitsutoyo, Tokyo). Mean value and
SE were calculated with a processor (DP-1HS, Mitsutoyo).
Light Treatment
LEDs were used to develop a new irradiation system consisting of
600 R-LEDs (EBR5305S, Stanley Electronics, Tokyo; peak emission at 660 nm, halfwidth in 30 nm, maximum output of 2 mW) and 200 FR-LEDs
(HE7601S, Hitachi, Tokyo; peak emission at 770 nm, halfwidth in 50 nm,
maximum output of 30 mW). The LEDs were mounted on a clear
polycarbonate board (20 × 26 cm) in rows (24 rows for R-LED arrays and six rows for FR-LED arrays). Each array contained 33 R-LEDs
or FR-LEDs spaced 3.0 mm apart. Duration of pulses of R or FR light and
their photon fluence rate were separately controlled by the electrical
system. Photon fluence rate was measured using the optical power meter
(1830-C, Newport, Irvine, CA). Maximum outputs generated from the LED
irradiation system were 2.2 mW cm 2 for R light
(corresponding to 120 µmol m 2
s 1 at 650 nm) and 12 mW
cm 2 for FR light (corresponding to 1.2 mmol
m 2 s 1 at 770 nm),
respectively. General characteristics of the LED irradiation system for
plants were reviewed elsewhere (Bula et al., 1991 ).
Determination of Action Spectra
Intermittent irradiation with monochromatic light for 1 min with
intervals of 2 min of darkness was carried out using the Okazaki large
spectrograph (Watanabe et al., 1982 ). Fluence-response curves in the
phyB mutant and the phyAphyB mutant were
determined at 20 different wavelengths from 320 to 780 nm at intervals
of 10 to 67 nm. Action spectra for 20% inhibition of hypocotyl
elongation at each wavelength were constructed from these curves.
Photon effectiveness was calculated as the reciprocal of the fluence required for 20% inhibition of hypocotyl elongation, which is represented by 80% relative hypocotyl length to the dark level obtained from the fluence response curves.
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RESULTS |
Effects of Intermittent Irradiation with FR Light
First we tested whether the effect of continuous FR irradiation on
inhibition of hypocotyl elongation in the wild type and the
phyB mutant of Arabidopsis could be replaced by intermittent irradiation with FR light pulses. Two-day-old etiolated seedlings were
exposed intermittently to FR light pulses (180 µmol
m 2 s 1 for 10 s)
for 5 d (Fig. 1A), and the hypocotyl
lengths were measured. The seedlings grown under FR light pulses at
intervals of 3 min or shorter showed equivalent hypocotyl lengths as
the seedlings grown in continuous FR irradiation (Fig. 1B). In
contrast, when the seedlings were grown under FR light pulses at
intervals of 15 min or longer, their hypocotyl lengths were
indistinguishable from those of the dark-grown seedlings (Fig. 1B). The
phyA mutant and the phyAphyB mutant did not show
hypocotyl shortening under any of these conditions (Fig. 1B). These
results indicated that intermittent irradiation with FR light at
intervals of 3 min or less caused an equivalent effect on
PhyA-dependent inhibition of hypocotyl elongation, as did continuous FR
irradiation.

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Figure 1.
Effect of intermittent irradiation with FR light
on PhyA-mediated inhibition of hypocotyl elongation in Arabidopsis. A,
Light regime. Two-day-old etiolated seedlings were transferred to
intermittent FR light irradiation of various cycles, continuous FR
light, or darkness and grown for 5 d, and their hypocotyl lengths
were measured. Long white bar, Continuous irradiation with FR light (30 µmol m 2 s 1); long black bars, continuous
darkness; small white boxes, intermittent irradiation, FR light pulses
(180 µmol m 2 s 1 for 10 s each) with
LEDs. B, Responses to intermittent irradiation with FR light in
wild-type (WT, ), phyA ( ), phyB
( ), and phyAphyB ( ) mutants. Values at a dark
interval of 0 min correspond to continuous irradiation. Error bars
represent SE.
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To determine whether the process of photoperception obeyed the
Bunsen-Roscoe law of reciprocity, the response was measured after
changing either the exposure time of cyclical FR light pulses or the
total light energy using the 3-min cyclical irradiation regime (Fig.
2A). The wild-type seedlings showed an
inhibition of hypocotyl elongation proportional to the total light
energy per pulse across the range of photon fluences from 0.04 to 2 mmol m 2 (Fig. 2B, WT). The response did not
show any dependency either on the exposure time within the range
examined (1-60 s) or on the photon fluence rate (0.62-620 µmol
m 2s 1) (Fig. 2B, WT).
Essentially the same results were obtained with phyB mutant
seedlings (Fig. 2B, phyB). Therefore, the Bunsen-Roscoe law
of reciprocity held in this response, suggesting that photoperception by PhyA is a rate-limiting factor of this response.

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Figure 2.
Relationship between the hypocotyl length and the
photon fluence of FR light per pulse. A, Light regime. Two-day-old
etiolated seedlings of the wild type were transferred and grown in the
intermittent irradiation with different intensities of FR light for
different durations of exposure time in 3-min cycles for 5 d, and
their hypocotyl lengths were measured. White bars, FR light pulses with
LEDs; black bars, darkness. B, Responses to intermittent irradiation
with FR light pulses for 1 s ( ), 3 s ( ), 10 s
( ), and 60 s ( ) in the wild type (top graph) and the
phyB mutant (bottom graph). Error bars represent
SE.
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Effects of Duration of Intermittent FR Light Treatment on Hypocotyl
Growth
To find how long prolonged irradiation with FR light is needed for
detection of this response, the phyB mutant seedlings were grown under continuous FR light (90 µmol m 2
s 1) for various durations from 5 min to 24 h and then kept in darkness for 5 d. Their hypocotyl lengths were
measured and compared with those of the seedlings treated with
continuous irradiation with FR light for 6 d as a control. In
treatments 12 h or shorter, the hypocotyls were not as short as
those of seedlings treated with continuous irradiation for 6 d
(data not shown). When the seedlings were exposed to continuous FR
light for 24 h, the hypocotyls were as long as those of seedlings
treated with continuous irradiation for 6 d (data not shown).
The time courses of hypocotyl elongation in seedlings grown under
intermittent FR irradiation were examined. When 2-d-old wild-type
seedlings were grown under intermittent irradiation with FR light
pulses (100 µmol m 2
s 1 for 10 s) for 24 h, the time
course of hypocotyl elongation was the same as the seedlings that were
given intermittent FR irradiation throughout their hypocotyl growth
(for several days) (Fig. 3B, WT). For
both of these treatments, the hypocotyl growth rate increased during
the 1st d from the beginning of the irradiation, and then decreased,
reaching its maximum within 4 d after induction of germination
(Fig. 3B, WT). In contrast, the hypocotyls of dark-grown seedlings
continued to elongate until the 7th d after induction of germination
(Fig. 3, WT). Essentially similar time courses of hypocotyl elongation
were obtained in the phyB mutant seedlings, although the
final hypocotyl length of the seedlings treated with FR light pulses
for 24 h was slightly longer than in those treated with FR light
pulses throughout their hypocotyl growth (Fig. 3B, phyB).
These results show that, in either continuous or intermittent irradiation, FR irradiation of just 24 h can cause the equivalent effect on inhibition of hypocotyl elongation obtained by prolonged (more than 2 d) FR irradiation.

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Figure 3.
Effect of intermittent irradiation with FR light
pulses for 1 d on further growth of the hypocotyl in darkness. A,
Light regime. Two-day-old etiolated seedlings were treated as follows:
one group ( ) was kept under intermittent irradiation with FR light
pulses (100 µmol m 2 s 1 for 10 s
each) in 3-min cycles throughout the experiment, the second group ( )
was exposed to the same intermittent FR light irradiation for 1 d,
then grown in the dark, the third group ( ) was kept in the dark, and
the fourth group ( ) was kept under continuous irradiation with FR
light (5.6 µmol m 2 s 1) for 9 d.
White lines in black bars, FR light pulses with LEDs; black bars,
darkness; white bars, continuous irradiation with FR light. B, Time
courses of the hypocotyl growth in the wild type (top graph) and the
phyB mutant (bottom graph). Error bars represent
SE.
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Action Spectrum for PhyA-Dependent HIR of Hypocotyl Elongation
As the photoperception by PhyA under the intermittent irradiation
conditions obeyed the Bunsen-Roscoe law of reciprocity (Fig. 2), we
were able to analyze the relative efficacy of different wavelengths of
light for inducing equivalent hypocotyl inhibition responses. The
Okazaki large spectrograph and its threshold boxes were designed and
built so that monochromatic lights are intermittently exposed in
desired fluence rates at wavelengths of 250 to 1,000 nm (Watanabe et
al., 1982 ). Etiolated seedlings with hypocotyls shorter than 2 mm were
intermittently irradiated with monochromatic light in 3-min cycles for
24 h, then kept in darkness for 5 d, and their hypocotyl
lengths were measured. Hypocotyl lengths were normalized to hypocotyl
lengths of dark controls and plotted against the photon fluence per
pulse to generate fluence response curves at each wavelength (Fig.
4). Based on the fluence-response curves, the photon fluences required for 20% inhibition of hypocotyl
elongation were determined at each wavelength, and their reciprocals
were plotted to construct the action spectra (Fig.
5).

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Figure 4.
Effect of intermittent irradiation with 320 to 780 nm of light on inhibition of hypocotyl elongation in the
phyB and the phyAphyB double mutants.
Two-day-old etiolated seedlings of the phyB mutant ( )
and the phyAphyB double mutant ( ) were exposed to
intermittent irradiation with monochromatic light in 3-min cycles for
1 d, then grown in the dark for 5 d, and their hypocotyl
lengths were measured. Error bars represent SE.
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Figure 5.
Action spectra for inhibition of hypocotyl
elongation in the phyB and the phyAphyB
double mutants by intermittent light treatment. Photon effectiveness
for the response was calculated as reciprocal of the fluence required
for 20% inhibition of hypocotyl elongation based upon the data in
Figure 4. The area shaded gray in the figure corresponds to the
differences between the spectrum of the phyB mutant
( ) and the phyAphyB double mutant ( ), and is due
to the involvement of PhyA for the response.
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We performed this analysis for the phyB and
phyAphyB mutants. The difference between the action spectrum
for the response in the phyB mutant and that in the
phyAphyB mutant (Fig. 5, shaded region) was attributed to
the deficiency of PhyA in the absence of PhyB. The action spectrum for
20% inhibition of hypocotyl elongation in the phyB mutant
showed a range of effective wavelengths, with two regions occurring at
690 to 750 nm and 320 to 500 nm (Fig. 5). In contrast, the action
spectrum in the phyAphyB mutant showed no effectiveness in
the 500- to 750-nm region, but retained the peak in the UV-A to blue
light region, although this was less effective than in the
phyB mutant (Fig. 5). Neither of the mutants responded to
550 to 667 nm of light within the range of the photon fluences examined
(Fig. 4).
The results indicated that PhyA perceived both FR light (690-750 nm)
and UV-A to blue light (320-500 nm) and effectively mediated inhibition of hypocotyl elongation. In contrast, intermittently exposed
R light (550-667 nm) induced no effect on PhyA-dependent hypocotyl
elongation. The effective range of the resultant action spectra in vivo
(Fig. 5) were within the effective range for the photoconversion from
Pfr to red-absorbing phytochrome (Pr) in vitro (Butler et al., 1959 ;
Furuya and Song, 1994 ; Mancinelli, 1994 ).
Photoreversible Effect of Intermittent R and FR Light Pulses
A question arose whether the effect of FR light pulses on
hypocotyl elongation could be canceled by R light pulses given
immediately after each FR light pulse in 3-min cycles. In the
phyB mutant, irradiation with R light pulses given
immediately after each FR light pulse caused hypocotyls to elongate as
much as those of dark-grown seedlings (Table
I, phyB-1). Consecutive
exposure of FR light following FR and R light pulses resulted in
hypocotyls as short as (or shorter than) those treated with FR light
pulses alone (Table I, phyB-1). The phyAphyB
double mutant showed no such photoreversible responses (Table I,
phyAphyB). These results indicated that photoperception of
each cycle is a photoreversible process mediated by PhyA.
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Table I.
Effect of intermittent consecutive FR and R light
pulses on hypocotyl elongation in wild-type, phyA, phyB, and phyAphyB
mutants
Two-day-old etiolated seedlings were transferred to intermittent
irradiation with R light (2 mmol m 2) and/or FR light (5 mmol m 2) pulses in 3-min cycles using the LED irradiation
system, grown for 5 d, and their hypocotyl lengths were measured.
Values are means of 30 seedlings ± SE.
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In contrast, the phyA mutant showed reversible responses in
the opposite manner to the phyB mutant; namely, R light
pulses inhibited hypocotyl elongation, and complete R/FR light
reversibility was observed in the 3-min cyclical irradiation (Table I,
phyA-201).
In wild-type seedlings, both FR and R light pulses in any combination
resulted in shorter hypocotyls than those of dark-grown seedlings
(Table I, WT). Interestingly, the hypocotyl lengths of the wild type
caused by irradiation with FR light pulses or FR/R/FR light pulses were
not significantly different from those of the phyB mutant
(Table I), although the effects of R and FR light on the PhyA- and
PhyB-dependent inhibition of hypocotyl elongation are opposite.
Similarly, the hypocotyl length of the wild type caused by irradiation
with R light pulses or FR/R light pulses were not significantly
different from those of the phyA mutant (Table I). These
results suggest that the PhyA-dependent inhibition of hypocotyl
elongation by irradiation with FR light, and the PhyB-dependent
inhibition of hypocotyl elongation by irradiation with R light do not
interfere with each other in wild-type seedlings.
Essentially similar results were obtained with wild-type seedlings of
ecotype Columbia and phyB-9 mutant seedlings (Columbia background) treated with intermittent FR and R light pulses (data not shown).
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DISCUSSION |
Photoconversion of PhyA from Pfr to Pr Induces FR
Light-Mediated HIR
The results presented in this paper show that both PhyA- and
PhyB-dependent HIR of hypocotyl inhibition responses are
photoreversible, and that R and FR light act in opposite directions in
responses mediated by the two photoreceptors. To our knowledge, this is the first description of a R/FR-light-reversible regulation of PhyA-mediated FR-HIR.
Our results lead us to a hypothesis that the PhyA-mediated HIR is
induced by a signal that is transmitted during photoconversion from Pfr
to Pr, and that neither dark-synthesized Pr nor photoconverted Pfr is
effective. First, PhyA in Pr synthesized in seedlings in darkness
showed no ability to induce HIR, because the presence or absence of
PhyA did not affect the elongation of hypocotyl length in darkness
(Table I), as was reported previously (Nagatani et al., 1993 ; Reed et
al., 1994 ). Second, the evidence that R light (550-667 nm) pulses
alone had no effect (Fig. 4) strongly suggested that the PhyA in Pfr
does not induce this response. Third, the effective range of wavelength
in the action spectrum for PhyA-dependent HIR of inhibition of
hypocotyl elongation by intermittent light (Fig. 5) were within the
effective range of wavelength in the absorption spectrum of Pfr (Butler
et al., 1959 , 1964 ; Furuya and Song, 1994 ). In contrast, the effective
range of wavelengths in FR light region in the action spectrum were outside the range of the absorption spectrum of Pr. Fourth, the effect
of FR light pulses on the response was repeatedly reversed by R light
pulses (Table I). Fifth, intermittent irradiation with FR/R/FR light
pulses led to significantly greater effect on inhibition of hypocotyl
elongation than that with just FR light pulses in both the wild type
and the phyB mutant (Table I). This finding is explained by
the speculation that irradiation with FR/R/FR light pulses generates a
relatively larger pool of photocycled Pr than irradiation with FR light
pulses alone does. These results allow us to construct a simple model
of PhyA action showing that this response correlates with the
photoperception of PhyA in Pfr producing Pr, rather than the
photoperception of Pr producing Pfr.
Over the last 4 decades, many scientists in this field have believed
that Pfr is the only biologically active form of the molecule, although
the reliability of this concept was questioned (Smith, 1983 ). Most of
the action spectra for FR-HIR reported were constructed from data
obtained under continuous irradiation before appreciation of the
existence of a family of phytochromes (Mohr, 1962 ; Mancinelli, 1994 ).
They showed effective ranges at 420 to 500 nm and 710 to 750 nm,
and their spectrum peaks fluctuated depending on materials; peaks at
420, 450, and 728 nm (Mohr and Wehrung, 1960 ) or at 370, 440, and 716 nm (Hartmann, 1967 ) in inhibition of hypocotyl elongation in dark-grown
lettuce seedlings, and at 450 and 730 nm in reopening of the plumular
hook in lettuce seedlings (Mohr, 1962 ). They did not show a simple
correlation with the photoconversion from Pr to Pfr or from Pfr to Pr
(Mohr, 1962 ; Hartmann, 1967 ; Mancinelli, 1994 ).
To explain those action spectra, many models for FR-HIR were proposed
based on the molecular properties of phytochromes, including balances
of biosynthesis, photoconversion, and degradation of phytochrome pools
(Smith, 1970 ; Mohr, 1972 ; Schäfer, 1975 ; Johnson and Tasker,
1979 ). The application of intermittent irradiation for
phytochrome-deficient mutants directed us to a model and interpretation
based on the specific function of the phytochrome family for the action
spectrum of FR-HIR (Fig. 5).
Recently, a positive function of Pr was suggested (Reed, 1999 ) by
studies of phytochrome-dependent seed germination (Reed et al., 1994 ;
Shinomura et al., 1994 ), morphogenesis in darkness (Kim et al., 1998 ),
and autophosphorylation of phytochromes (Yeh et al., 1997 ; Yeh and
Lagarias, 1998 ). Autophosphorylation of cyanobacterial phytochrome was
promoted by continuous FR irradiation (when Pr should predominate)
rather than by continuous R irradiation (when Pfr should predominate)
(Yeh et al., 1997 ). In oat phytochrome, Pfr (Sommer et al., 1996 ) and
also Pr (Yeh and Lagarias, 1998 ) were phosphorylated. The phytochrome
action model (Yeh and Lagarias, 1998 ) based upon those molecular data
is consistent with the idea from the present physiological study that
photoconversion of PhyA into Pr by FR light perception promotes a
biologically active signal.
PhyA Signal for HIR Is Short-Lived
The PhyA-dependent signal produced by photoconversion from Pfr to
Pr appears to be short-lived because the effect of FR light pulses
disappeared within 15 min (Fig. 1).In contrast, the PhyB-produced signal for HIR is stable because the effect of R light pulses persisted
for 4 h (McCormac et al., 1993 ; Ahmad and Cashmore, 1997 ).
Previously, before the existence of a family of phytochromes was known,
it was found that induction of anthocyanin production by intermittent
FR light pulses at intervals of a few minutes or shorter brought about
the equivalent extent of the response as continuous FR light
irradiation in milo seedlings (Downs and Siegelman, 1963 ) and in
cabbage and mustard seedlings (Mancinelli and Rabino, 1975 ). The common
requirement for frequent irradiation with FR light pulses for induction
of these responses strongly suggests that the effects of intermittent
FR light pulses in anthocyanin production resulted from PhyA action.
These results remind us of the existence of two pools of
physiologically stable phytochrome and labile phytochrome in plant tissues (Furuya, 1989 ). Pfr of type II phytochrome, including PhyB and
probably other phytochromes, is stable in the dark for long periods,
for years in dry seeds, and then induces responses. In contrast, Pfr of
Type I phytochrome, which corresponds to PhyA, is unstable and
disappears rapidly after irradiation with R light in the subsequent
dark period (Takimoto and Saji, 1984 ). However, the time course of
disappearance of the effectiveness of each FR light pulse in the
present study (Fig. 1) is faster than the time course of phytochrome
degradation (Vierstra, 1994 ) or dark reversions (Briggs and Rice, 1972 )
previously reported. Therefore, it is still an open question whether
the labile nature of PhyA contributes to the requirement of frequent FR
light exposure in PhyA-dependent HIR.
Although rapid degradation is generally assumed to be specific to
Pfr (Vierstra, 1994 ), rapid degradation of Pr (one-half of the pool
degraded within 4 h) was observed under specific conditions in
etiolated oat (Chorney and Gordon, 1965 ; Stone and Pratt, 1979 ). Degradation of Pr required that dark-synthesized Pr is converted to Pfr
and then back to Pr for generating photocycled-Pr (Chorney and Gordon,
1965 ; Stone and Pratt, 1979 ). This requirement for Pr cycling is
similar to that for PhyA-mediated HIR in Arabidopsis, but further
analysis for physiological role of photocycled Pr degradation in PhyA
is needed to conclude whether these two phenomena are related or not.
Another question arises whether the "photoconverted Pr" of PhyA is
directly responsible for the induction of the response, or whether some
"intermediate form(s)" of PhyA produced in photoconversion from Pfr
to Pr (Bischoff et al., 1998 ) is responsible. Two possibilities may
explain the short-lived PhyA signal: (a) Pr itself is responsible for
the response but its activity disappears rapidly for an unknown reason,
or (b) some unstable intermediate form produced by photoconversion from
Pfr to Pr is responsible for the induction of the response. Various
approaches have been applied to study the molecular and kinetic
mechanisms that occur in the course of the Pr to Pfr
phototransformation (Furuya, 1983 ; Rüdiger and Thümmler,
1994 ). In contrast, the back reaction from Pfr to Pr has not been as
thoroughly investigated (Bischoff et al., 1998 ).
PhyA-Mediated HIR Is Fluence Dependent
It was well established that two of the defining characteristics
of the FR-HIR are the requirement for prolonged irradiation and the
dependency upon fluence rate (Briggs et al., 1984 ; Mancinelli, 1994 ).
The present study revealed that for either intermittent or
continuous irradiation, maximal inhibition of hypocotyl
elongation mediated by PhyA is achieved during the first 24-h
irradiation with FR light (Fig. 3). Although the reason why a minimum
of 24 h of irradiation is still required to elicit the response is
obscure, we speculate that a 24-h irradiation period leads to an
irreversible change in hypocotyl growth rate that persists for several
days in the absence of any further light stimulus.
The photon fluence dependency for PhyA-mediated FR-HIR by intermittent
irradiation may also explain why the FR-HIR by continuous irradiation
depends on the fluence rate. The present study revealed that the extent
of inhibition of hypocotyl elongation mediated by PhyA shows a linear
correlation with photon fluence per each FR light pulse they are given
at intervals of 3 min or shorter (Figs. 1 and 2). If the duration of FR
light pulse is extended to 3 min, which corresponds to "continuous
irradiation," an increase of fluence rate inevitably causes an
increase of photon fluence. Under such continuous irradiation, the
extent of the response appears to depend on fluence rate, but actually
depends on photon fluence in each elementary process of photoperception
by PhyA. In fact, in the wild type and the phyB mutant,
similar inhibition of hypocotyl length was achieved by both continuous
and intermittent irradiation if the same photon fluence (1 mmol
m 2) was used during each 3 min (Fig. 3).
PhyA Cues Responses by Two Distinct Modes of Photoperception
The present study demonstrated conclusively, for the first time to
our knowledge, that PhyA in Arabidopsis has at least two different
modes of photoperception, one observed in "photoirreversible" VLFR
and depending on the photoconversion from Pr to Pfr (Shinomura et al.,
1996 ; Hamazato et al., 1997 ), and another, found here, observed in
"FR/R light photoreversible" HIR depending on the photoconversion
from Pfr to Pr. In PhyA-mediated VLFR of seed germination in
Arabidopsis, either a pulse of FR light (1 µmol m 2 and higher of 726 nm of light) or a pulse of
very low fluence of R light (1 nmol m 2 and
higher of 667 nm of light) induced germination, and photoreversibility was not reported (Shinomura et al., 1996 ). The action spectrum for this
response correlated well with the absorption spectrum of Pr (Shinomura
et al., 1996 ), demonstrating that the concept of Pfr as the active form
of phytochrome was consistent with that physiological response. On the
other hand, in PhyA-mediated HIR of inhibition of hypocotyl
elongation, only FR light pulses (66 µmol m 2
and higher of 726 nm of light each, Fig. 4) induced the response, but R
light pulses given alone never induced this response.
The modes of photoperception by PhyA for HIR and VLFR are different
from that for PhyB-mediated responses, although PhyA and PhyB have
similar absorption spectra in vitro (Abe et al., 1989 ; Kunkel et al.,
1993 ), amino acid sequences (Sharrock and Quail, 1989 ), and protein
subdomain structures (Xu et al., 1995 ; Wagner et al., 1996 ). These
results suggest that the PhyA-dependent inhibition of hypocotyl
elongation may represent a specialized branch of the FR/R light sensing
pathway, with unique transduction components not shared by other
photoreceptors. This idea would help to explain many complicated
physiological characteristics of the photoinhibition of stem elongation
reported so far.
The ecological significance of phytochromes as spectral sensors for
growth and photosynthesis has been well characterized and discussed in
relation to the physiological function of phytochromes and their R/FR
light reversible characteristics, but the significance of FR-HIR has
been obscure (Smith, 1994 ). Interestingly, the present study showed
that both R and FR light are effective for the inhibition of hypocotyl
elongation in wild-type Arabidopsis (Table I). Given that FR
irradiation causes simultaneous production of Pr in both PhyA and PhyB,
it appears that the primary function of PhyA for the response was
unaffected by PhyB in wild-type seedlings. Similarly, the primary
function of PhyB by photoconversion into Pfr by irradiation with R
light pulses was unaffected by PhyA of Pfr in the wild-type seedlings.
These results reveal that plants use the overlapping functions of PhyA
and PhyB separately, and have evolved different modes of action for the
different phytochromes in order to occupy a greater variety of niches
in the light landscape.
 |
ACKNOWLEDGMENTS |
We thank Pill-Soon Song and Jason W. Reed for insightful
discussions; Norio Murata and Masakatsu Watanabe for hosting us at the
National Institute for Basic Biology; Mamoru Kubota and Sho-ichi Higashi for help with operation of the Okazaki large spectrograph; Kenya Suzuki for the physiological experiment; Takao Yokota for discussion and support; Masashi Kiguchi for helpful advice on calculation of optical power; Ryoko Katayanagi for greenhouse plant
care; Sigeo Kubota and Hiroshi Tohyama for building the LED irradiation
system; and laboratory staff for discussion and support.
 |
FOOTNOTES |
Received May 24, 1999; accepted September 14, 1999.
1
This work was carried out under Hitachi Advanced
Research Laboratory project (no. B2023) and National Institute for
Basic Biology Cooperative Research Program for the Okazaki large
spectrograph (grant nos. 97-524 and 98-522). Research was partly
supported by a grant from the Program for Promotion of Basic Research
Activity for Innovative Biosciences to M.F.
2
This paper is dedicated to Hans Mohr who had
made the greatest contribution to HIR.
*
Corresponding author; e-mail mfuruya{at}harl.hitachi.co.jp; fax
81-492-96-7511.
 |
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