Resonance Raman and Ligand Binding Studies of the Oxygen-sensing
Signal Transducer Protein HemAT from Bacillus subtilis*
Shigetoshi
Aono
§,
Toshiyuki
Kato
,
Mayumi
Matsuki
,
Hiroshi
Nakajima
,
Takehiro
Ohta¶,
Takeshi
Uchida¶, and
Teizo
Kitagawa¶
From the
School of Materials Science, Japan Advanced
Institute of Science and Technology, 1-1 Asahidai, Tatsunokuchi,
Ishikawa 923-1292 and the ¶ Center for Integrative Bioscience,
Okazaki National Research Institutes, Myodaiji, Okazaki, Aichi
444-8585, Japan
Received for publication, December 21, 2001
 |
ABSTRACT |
HemAT-Bs is a heme-containing signal transducer
protein responsible for aerotaxis of Bacillus subtilis. The
recombinant HemAT-Bs expressed in Escherichia coli was
purified as the oxy form in which oxygen was bound to the ferrous heme.
Oxygen binding and dissociation rate constants were determined to be
kon = 32 µM
1
s
1 and koff = 23 s
1, respectively, revealing that HemAT-Bs has a moderate
oxygen affinity similar to that of sperm whale myoglobin (Mb). The rate constant for autoxidation at 37 °C was 0.06 h
1, which
is also close to that of Mb. Although the electronic absorption spectra
of HemAT-Bs were similar to those of Mb, HemAT-Bs showed some unique
characteristics in its resonance Raman spectra. Oxygen-bound HemAT-Bs gave the
Fe-O2
band at a noticeably low frequency (560 cm
1), which
suggests a unique hydrogen bonding between a distal amino acid
residue and the proximal atom of the bound oxygen molecule. Deoxy
HemAT-Bs gave the
Fe-His band at a higher
frequency (225 cm
1) than those of ordinary
His-coordinated deoxy heme proteins. CO-bound HemAT-Bs gave the
Fe-CO and
C-O bands at 494 and 1964 cm
1, respectively, which fall on the same
C-O versus
Fe-CO correlation line as that of Mb. Based on these results, the structural and functional properties of HemAT-Bs are discussed.
 |
INTRODUCTION |
Motile bacteria are known to swim toward or away from specific
environmental stimuli such as nutrients, oxygen, or light (1, 2). This
behavior, termed chemotaxis, is mediated by a signal transduction
system consisting of methyl-accepting chemotaxis proteins
(MCPs),1 a histidine kinase
CheA, a response regulator CheY, a coupling protein CheW, and the two
enzymes that mediate sensory adaptation by covalently modifying the
MCPs, CheR and CheB (3-6). Typical MCP is an integral membrane protein
with an N-terminal periplasmic substrate binding domain and a
C-terminal cytoplasmic signaling domain (7, 8). The binding of a
substrate, a repellent, or attractant to the periplasmic substrate
binding domain is believed to induce a change in the MCP conformation
that allows it to activate CheA (7, 8). The activated CheA
phosphorylates CheY, and, consequently, the phosphorylated CheY binds
to the switch complex at the base of the flagella to control the
direction of flagellar rotation (3-6). In this signal transduction
system, MCP acts as a sensor for the external signal and as a signal transducer.
Hou et al. (9) have recently reported that Bacillus
subtilis and Halobacterium salinarum have a signal
transducer protein, HemAT-Bs and HemAT-Hs, respectively, for
aerotaxis, the migratory response toward or away from oxygen.
HemAT-Bs and HemAT-Hs are soluble proteins, and their
C-terminal regions, residues 222-489 of HemAT-Hs and 198-432
of HemAT-Bs, are 30% identical to the cytoplasmic signaling domain of
Tsr, an MCP from Escherichia coli (9). Their N-terminal
regions, residues 1-184 in HemAT-Hs and 1-175 in HemAT-Bs, show
limited homology to myoglobin (9). Recombinant HemAT-Bs and HemAT-Hs
are hemoproteins containing a b-type heme as a prosthetic group and
show similar electronic absorption spectra to those of myoglobin (9).
HemAT-Bs and HemAT-Hs bind oxygen reversibly as myoglobin does. The
residues 1-195 for HemAT-Hs and 1-176 in HemAT-Bs retain the heme-
and oxygen-binding properties of the respective native proteins, which represent a globin-coupled sensor motif (10). These results suggest
that the heme in HemAT acts as an oxygen sensor and that the binding of
oxygen to the heme in HemAT triggers the signal transduction for
aerotaxis in B. subtilis and H. salinarum.
Sensing gas molecules such as O2, NO, and CO is a novel
function of hemoproteins (11-14), whereas hemoproteins exhibit a wide variety of functions such as oxygen storage/transport, electron transfer, and redox reactions of various substrates. Recently, reports
on hemoprotein sensors in which a heme prosthetic group acts as a
sensor for a gas molecule such as O2, NO, or CO are on the
increase. FixL (15), direct oxygen sensor (16), and phosphodiesterase A1 (17) for O2 sensors, soluble guanylate cyclase (sGC) (18) for a NO sensor, and CooA (19-21) for a CO sensor
are typical examples for hemoprotein sensors. In these sensor proteins,
the binding of O2, NO, or CO to the heme regulates the
function of these proteins. The hemes in these sensor proteins play a
central role not only for sensing their effector molecules but also for
regulating the functional properties with a conformational change
induced by the ligand binding.
The heme in HemAT is thought to be the active site for sensing
O2, and the binding of O2 to the heme will be
responsible for triggering the aerotaxis signal transduction.
Therefore, the elucidation for the coordination structure of the heme,
especially in the O2-bound form and for the interaction
between the bound O2 and the heme pocket, are required to
understand the mechanism of the O2 sensing and signal
transduction for HemAT. Although the electronic absorption spectra of
HemAT-Hs and HemAT-Bs are reported (9), very little information is
available for the structure and ligand binding properties of the heme
in HemAT. In this work, we present results of the kinetic analysis for
oxygen binding with HemAT-Bs, autoxidation kinetics of oxygen-bound
HemAT-Bs, and resonance Raman measurements with the deoxy, oxy, and
CO-bound forms of HemAT-Bs. Using resonance Raman spectroscopy, we show
a unique heme environment for HemAT-Bs.
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EXPERIMENTAL PROCEDURES |
Expression of HemAT-Bs in E. coli--
An expression vector for
HemAT-Bs was constructed as follows. The
hemAT-Bs gene was prepared by polymerase chain reaction (PCR) with the chromosomal DNA of B. subtilis and the two
synthetic deoxyoligonucleotides
(5'-gaaggagatccatatgttatttaaaaaagacagaaaacaagaaacagc-3' and
5'-ggatcccatatgttattattcttctgtcaggatgacaagcgaatcaacgg-3' for the sense
and antisense primers, respectively) as the template and primers,
respectively. Although the original translational initiation codon for
HemAT-Bs is TTG in B. subtilis (9), the translational
initiation codon was changed to ATG in the sense primer, which is
underlined in the above sequence. The PCR product was cloned into a
pCR4-TOPO vector with the TOPO TA cloning kit (Invitrogen). The plasmid
containing the hemAT-Bs gene with the correct direction
relative to the lac promoter was selected as an expression
vector for HemAT-Bs and named pCR-HemAT.
E. coli JM109 was used as a host for the expression of
HemAT-Bs. pCR-HemAT/E. coli JM109 was grown in LB medium
containing 50 µg/ml ampicillin at 37 °C. The expression of
HemAT-Bs was induced by 1 mM
isopropyl-
-D-thiogalactopyranoside. The cultivation was continued at 25 °C for 12 h after adding
isopropyl-
-D-thiogalactopyranoside. The cells were
harvested by centrifugation and stored at
80 °C until use.
Purification of the Recombinant HemAT-Bs--
Purification of
the recombinant HemAT-Bs was carried out as follows. The cells were
resuspended in 50 mM Tris-HCl buffer, pH 8.5, containing 1 mM phenylmethylsulfonyl fluoride and disrupted by
sonication. After unbroken cells and cell debris were removed by
centrifugation, the supernatant was applied to a column (2.6 × 30 cm) of Q-Sepharose (Amersham Biosciences, Inc.) equilibrated with 50 mM Tris-HCl buffer, pH 8.5. The adsorbed proteins were eluted by a linear gradient of NaCl from 0 to 0.6 M at a
flow rate of 1 ml/min after washing the column with a 4-bed volume of
50 mM Tris-HCl buffer, pH 8.5. The fractions containing
HemAT-Bs were combined and applied to a column (1.6 × 30 cm) of
hydroxylapatite (Seikagaku Co.) equilibrated with 50 mM
Tris-HCl containing 1 M KCl, pH 8.5. The adsorbed proteins
were eluted at a flow rate of 1 ml/min by increasing linearly the
concentration of K2HPO4 in the elution buffer
from 0 to 0.3 M. The fractions containing HemAT-Bs were
combined and concentrated by a Centricon 50 (Amicon). The concentrated
sample was applied to a column (1.6 × 80 cm) of Superdex 200 pg
(Amersham Biosciences, Inc.) equilibrated with 50 mM
Tris-HCl buffer containing 0.1 M NaCl, pH 8.5. The column was run at 0.2 ml/min using 50 mM Tris-HCl buffer
containing 0.1 M NaCl, pH 8.5, as an elution buffer. 1-2
mg of purified HemAT-Bs was obtained from approximately 10 g of
wet cells of pCR-HemAT/E. coli JM109.
Characterization of HemAT-Bs--
The reduction of HemAT-Bs was
carried out by adding a few grains of sodium dithionite into the
isolated HemAT-Bs. CO gas was introduced into HemAT-Bs solution by a
gas-tight syringe.
The type of the heme in HemAT-Bs was determined by the pyridine
ferrohemochrome method. The value of 34 mM
1
cm
1 at the absorption maximum of the
band for the
pyridine ferrohemochrome derived from the protoheme was used to
calculate the concentration of the heme in HemAT-Bs. Protein
concentration was determined by the Coomassie Protein Assay Reagent
(Pierce) or the Advanced Protein Assay Reagent (Cytoskeleton Inc.)
using bovine serum albumin as a standard.
The molecular mass of HemAT-Bs was determined by gel filtration, using
a Superdex 200-pg gel filtration column (1.6 × 80 cm). The system
was calibrated with
-amylase (molecular weight, 200,000), alcohol
dehydrogenase (150,000), bovine serum albumin (66,000), carbonic
anhydrase (29,000), and cytochrome c (12, 400), using 50 mM Tris-HCl buffer containing 0.1 M NaCl, pH
8.5, as the eluent. These proteins used in the calibration were
obtained from Sigma Chemical Co.
Spectral Measurement--
The electronic absorption spectra were
measured on a Hitachi U-3300 UV-visible spectrophotometer. Resonance
Raman spectra were obtained with laser excitation at 413.1 nm by a
Kr+ laser (Spectra Physics, model 2016). The excitation
light was focused into the cell, and the laser power was 1 milliwatt
(mW) at the cell for the oxy and deoxy forms of HemAT-Bs but 0.1 mW for
CO-bound HemAT-Bs so as to avoid photolysis of coordinated CO. The
sample solutions for the Raman measurements were sealed in quartz
cells, which were rotated at 500 rpm at room temperature. Typically, 30 µl of the sample aliquots containing 30 µM protein in
50 mM Tris-HCl buffer, pH 8.5, were put into the cell. The scattered light was dispersed with a single polychromator (Ritsu, DG-1000) equipped with a liquid nitrogen-cooled charge-coupled device
camera. The spectral slit width was 6 cm
1. Raman shifts
were calibrated using indene and an aqueous solution of potassium
ferrocyanide as frequency standards, providing accuracy of ±1
cm
1 for intense isolated lines.
Ligand Binding Kinetics--
The bimolecular on-rate
(kon) of oxygen was determined at room
temperature after photolysis of oxygen-bound HemAT-Bs,
HemAT-Bs(O2), with a 20-ns Nd-YAG laser pulse at 532 nm
(Quanta Ray GCR-3). A Xe-lamp (ILC Technology, LX-300) was used as a
monitor light source. The transient kinetic curves were observed at 433 nm, which were measured on a digital storage oscilloscope (Tektronix 11401).
The off-rate (koff) of oxygen was determined by
stopped-flow spectrophotometry (Unisoku USP-526) at room temperature.
About 3 µM HemAT-Bs(O2) was mixed with 5 mM sodium dithionite solution in 50 mM Tris-HCl
buffer, pH 8.0, as reported previously (22). The reaction was followed
at 413 nm.
Autoxidation of HemAT-Bs--
The rate of autoxidation of
HemAT-Bs(O2) was measured in 50 mM Tris-HCl
buffer (pH 8.5) at 37 °C under air. HemAT-Bs(O2) as isolated was maintained in an optical quartz cell with 1-cm optical path length at 37 °C, and spectra were recorded at regular intervals of time with an Hitachi U-3300 UV-visible spectrophotometer.
 |
RESULTS |
HemAT-Bs was expressed as a soluble hemoprotein in the
expression system constructed in this study. A nearly homogeneous
HemAT-Bs was obtained by column chromatography described under
"Experimental Procedures," as evident from SDS-polyacrylamide gel
electrophoresis (Fig. 1a). The
pyridine ferrohemochrome derived from HemAT-Bs gave the
band at 556 nm (data not shown), which means that HemAT-Bs contains a protoheme
(b-type heme) as a prosthetic group. The molecular mass of the purified
HemAT-Bs was estimated to be about 188 kDa by gel filtration (Fig.
1b), suggesting that the purified HemAT-Bs is a
homo-tetramer of an identical subunit (48.7 kDa).

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Fig. 1.
SDS-PAGE of purified HemAT-Bs
(a) and estimation of molecular weight by gel
filtration column chromatography (b). The
circle and squares represent HemAT-Bs and
standard proteins for molecular weight determination (1,
-amylase; 2, alcohol dehydrogenase; 3, bovine
serum albumin; 4, carbonic anhydrase; 5,
cytochrome c), respectively.
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Kinetics Constants for the Reaction of Ferrous HemAT-Bs with
Oxygen--
The binding of oxygen to the heme is the first and crucial
step of the oxygen sensing and signal transduction by HemAT-Bs. Therefore, elucidation of the oxygen binding properties is essential to
understand the functional properties of HemAT-Bs. In this work, the
reaction rate constants for oxygen binding and dissociation, kon and koff, were
determined by laser-flash photolysis and stopped-flow spectroscopies,
respectively. The kon and
koff values for HemAT-Bs thus determined were 32 µM
1 s
1 and 23 s
1, respectively, which were similar to those of sperm
whale Mb (Sw Mb) (Table I).
HemAT-Bs exhibits a moderate oxygen affinity, similar to that of
Sw Mb but different from another oxygen sensor protein FixL.
FixL exhibits an extremely low oxygen affinity due to a very low
kon value (kon = 0.14 µM
1 s
1), although the
koff of FixL is comparable to that of HemAT-Bs (Table I).
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Table I
Kinetics and equilibrium constants for the reaction of ferrous
HemAT-Bs with oxygen compared to those of other hemoproteins
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The dissociation equilibrium constant (Kd) given by
the ratio koff/kon for
HemAT-Bs was 719 nM (Table I), which is comparable to the
Km values of terminal oxidases for oxygen
respiration. That the Kd value of HemAT-Bs
for O2 is comparable to Km values of
terminal oxidases seems reasonable from the functional point of view
for HemAT-Bs. Because HemAT-Bs acts as an oxygen-sensing signal
transducer in aerophilic response of B. subtilis (9), it
should detect the most suitable oxygen concentration for the bacterium,
i.e. that for oxygen respiration. If HemAT-Bs has an
extremely high oxygen affinity as do Mt Hb, Asacaris Hb, and Synechocystis Hb (Table I), it
would be disadvantageous, because a signal transduction would occur to
induce chemotaxis toward a too low concentration of oxygen unsuitable
for oxygen respiration. The Kd value of 719 nM for HemAT-Bs, a moderate oxygen affinity, reveals that
HemAT-Bs can detect an oxygen concentration suitable for oxygen respiration.
Autoxidation of Oxy HemAT-Bs--
HemAT-Bs(O2) as
isolated showed a rate constant for autoxidation of 0.06 h
1 at 37 °C, which is similar to that of Sw
Mb (Table II). FixL, another oxygen
sensor protein, shows a 20- to 40-fold lager autoxidation rate constant
compared with that of HemAT-Bs (29, 30). The kinetics parameters for
autoxidation and oxygen binding are different between HemAT-Bs and
FixL, which suggests some qualitative difference in the heme
environmental structure between the two oxygen sensor proteins.
Electronic Absorption Spectra of HemAT-Bs--
The electronic
absorption spectra of HemAT-Bs are shown in Fig.
2. HemAT-Bs as isolated gave the
Soret,
, and
peaks at 414, 578, and 543 nm, respectively, as
shown in Fig. 2a. This spectrum is typical of
six-coordinate, low spin hemoproteins and resembles that of the oxy
form of Mb, as described previously (9). When CO was reacted with the
isolated HemAT-Bs without any reductant, CO-bound HemAT-Bs was formed
(data not shown). These results strongly suggest that HemAT-Bs is
purified as the oxy form in which O2 is bound to the
ferrous heme. Resonance Raman spectroscopy revealed that this was the
case, as described below. Upon deoxygenation with sodium dithionite,
HemAT-Bs showed a spectrum with the Soret peak at 431 nm and a single
peak at 563 nm in the Q-band region, as shown in Fig. 2b.
This spectrum is typical of five-coordinate, high spin ferrous
hemoproteins, which show the formation of deoxy HemAT-Bs. CO-bound
HemAT-Bs was formed upon the reaction of dithionite reduced HemAT-Bs
with CO, which showed the Soret,
, and
peaks at 422, 567, and
543 nm, respectively, as shown in Fig. 2c. These electronic
absorption spectra of HemAT-Bs were similar to those of Mb as reported
previously (9), which is consistent with the fact that the
N-terminal region of HemAT-Bs shows an amino acid sequence homology
to Mb (9). The values of the absorption maxima observed in this study
are slightly different from those reported in Ref. 9. Hou et
al. have noted from their absorption spectra the presence of a
significant population of deoxy species for both the CO- and
O2-bound forms of HemAT-Bs (9). In our preparation of
HemAT-Bs, however, such an incomplete ligand binding was not noticed,
which was confirmed by resonance Raman spectroscopy as described below.
These differences may cause the difference of the absorption maxima,
although the reasons of the difference are not clear at present.

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Fig. 2.
Electronic absorption spectra of oxy
(a), deoxy (b), and CO-bound HemAT-Bs
(c). HemAT-Bs was dissolved in 50 mM
Tris-HCl buffer, pH 8.5. HemAT-Bs as isolated was in the oxy form.
Deoxy HemAT-Bs was prepared by adding sodium dithionite into oxy
HemAT-Bs solution. CO was introduced into deoxy HemAT-Bs solution to
prepare CO-bound HemAT-Bs. The molar extinction coefficients for the
heme in HemAT-Bs are shown in this figure.
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The heme in HemAT-Bs is thought to play an important role for sensing
O2. The ligand conformation, the interaction between the
bound O2 and the amino acid residue(s) in the heme pocket, and/or the heme environmental structure will be responsible for triggering the signal transduction upon the O2 binding to
the heme in HemAT-Bs. To characterize these properties, we measured the resonance Raman spectra of HemAT-Bs in the oxy, deoxy, and CO-bound forms.
Resonance Raman Spectra of Oxy HemAT-Bs--
The resonance Raman
spectrum in the high frequency region (1300-1700 cm
1) of
HemAT-Bs(O2) is shown in Fig.
3a. In Table
III, the observed frequencies of the
major bands are compared with those of Mb (32, 33), heme-bound heme
oxygenase (32, 33), and gas-sensing hemoproteins such as the
O2, CO, and NO sensors of FixL (34-37), CooA (38-40), and
sGC (41-43), respectively.
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Table III
High frequency vibrational modes of the oxy, deoxy (sodium dithionite
reduced), and CO-bound forms of hemoproteins
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It is established that resonance Raman spectra in the high frequency
region contain a few marker bands sensitive to the oxidation state
(
4) and the spin and coordination states
(
2 and
3) of the heme iron (44).
HemAT-Bs(O2) gave two bands at 1471 and 1501 cm
1 in the
3 band region, indicative of a
mixture of five- and six-coordinate heme species. The relative
intensities of these bands depended on the laser power, i.e.
the intensity of the band at 1471 cm
1 due to a
five-coordinate heme increased as the laser power increased. These
results show that the bound O2 in HemAT-Bs(O2)
was photodissociated to form the five-coordinate form at the higher
laser power. Therefore, the band at 1501 cm
1 was assigned
to the
3 band of HemAT-Bs(O2). The
2 band of HemAT-Bs(O2) was observed at 1578 cm
1.
The
2 and
3 modes of
HemAT-Bs(O2) observed at 1578 and 1501 cm
1,
respectively, are slightly lower than the corresponding ones of
Mb(O2) (
2 = 1584 cm
1 and
3 = 1507 cm
1) (33) but coincide with the
corresponding ones of FixL(O2) (
2 = 1577 cm
1 and
3 = 1502 cm
1) (34).
Because the
2 and
3 frequencies are
linearly correlated with the Ct-N distance (distance between the center
and a nitrogen atom of a porphyrin ring) (45, 46), the lower
frequencies of the
2 and
3 modes in
HemAT-Bs(O2) may be indicative of an expanded porphyrin
core compared with Mb(O2), which is also suggested for
FixL(O2) (34).
The resonance Raman spectra of HemAT-Bs(O2) in
the low frequency region are shown in Fig.
4. The spectra of the
16O2- and 18O2-bound
forms of HemAT-Bs are shown in the top and
middle, respectively, and the
16O2-18O2 difference
spectrum is shown in the bottom. A large isotope shift was
observed for the band at 560 cm
1 where the derivative
pattern of the difference spectrum was observed. Therefore, this band
is assigned to the Fe-O2 stretching mode (
Fe-O2). However, the
peak-to-valley frequency difference in Fig. 4c is as large
as 26 cm
1, which is slightly larger than the frequency
shift expected for an Fe-O2 diatomic oscillator (23 cm
1). The 561 cm
1 band in Fig.
4a is broader than those of other bands, implying inhomogeneous broadening. Accordingly, a too large isotopic
frequency shift might be caused by the existence of more than two bands and the difference of their intensity distributions between
16O2 and 18O2
derivatives. Although this should be clarified in later studies, it is
no doubt that the 560 cm
1 band primarily involves the
Fe-O2 character.

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Fig. 4.
The isotope shift in the low frequency
resonance Raman spectra of HemAT-Bs(O2).
16O2 (a),
18O2 (b), and
16O2-18O2
(c) represent the Raman spectra of
HemAT-Bs(16O2),
HemAT-Bs(18O2), and
HemAT-Bs(16O2)-HemAT-Bs(18O2),
respectively.
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The ligand modes of various hemoproteins are listed in Table
IV. The ligand modes get resonance Raman
intensity from the electronic coupling of the ligand orbital to the
metal and porphyrin orbitals. In particular, the assignment of a
ligand-Fe stretching mode is useful, because it directly reflects the
strength of the Fe-ligand bond and thus the nature of interactions
of the ligand with the surrounding amino acid residues.
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Table IV
The frequencies of the Fe-His, Fe-CO, Fe-O2, and C-O
stretching modes of hemeproteins determined by resonance Raman and
infrared spectroscopy
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Resonance Raman Spectra of Deoxy HemAT-Bs--
The high frequency
resonance Raman spectrum of deoxy HemAT-Bs is shown in Fig.
3b. Deoxy HemAT-Bs showed the
2,
3, and
4 modes at 1558, 1469, and 1352 cm
1, respectively, at typical frequencies of the deoxy
form of five-coordinate heme species in the high spin state.
The resonance Raman spectrum of deoxy HemAT-Bs in the low frequency
region is shown in Fig. 5a.
The intense line at 225 cm
1, which was undetectable with
the O2- and CO-bound forms, was observed for deoxy
HemAT-Bs. In general, the Fe-His stretching Raman band of hemoproteins
is observable in the region of 200-250 cm
1 for the
five-coordinate ferrous species (52). We thus assign the 225 cm
1 band to the Fe-His stretching mode of deoxy HemAT-Bs.
This frequency is higher than that of deoxy Mb, and it will be
discussed later.

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Fig. 5.
The 200-400 cm 1 region
resonance Raman spectra of deoxy HemAT-Bs (a) and
HemAT-Bs(CO) (b) and (c). The
power of the 413.1-nm laser for the measurement of deoxy HemAT-Bs was 1 mW (a), whereas 5 mW (b) and 0.1 mW
(c) laser power were applied for HemAT-Bs(CO).
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Resonance Raman Spectra of CO-bound HemAT-Bs--
The resonance
Raman spectrum of CO-bound HemAT-Bs, HemAT-Bs(CO), in the high
frequency region is shown in Fig. 3c. HemAT-Bs(CO) was
photolabile and showed two
3 bands at 1468 and
1495 cm
1, corresponding to a five-coordinate, high spin
and a six-coordinate, low spin heme species, respectively. The former
species is thought to be formed by photodissociation of the bound CO
upon the laser excitation. Thus, the CO-bound form gives the
2,
3, and
4 bands at 1578, 1495, and 1368 cm
1, respectively. The
4
frequency of the CO-bound form (1368 cm
1) is lower than
that of the O2-bound form (1372 cm
1),
indicating that the heme itself distinguishes O2 from CO as a ligand. Because the
4 frequency becomes higher for a
heme with larger delocalization of
electrons from the
eg orbital of porphyrin to the
* orbital of the bound
ligand through the d
orbital of Fe, the electron
delocalization is larger for O2 than for CO.
The resonance Raman spectra of HemAT-Bs(CO) in the low frequency region
are shown in Fig. 5 (b and c). The 225 cm
1 band was also observed in HemAT-Bs(CO) under
increased laser power conditions, as shown in Fig. 5b. This
suggests that photodissociation of CO from HemAT-Bs(CO) generates a
five-coordinate ferrous HemAT-Bs, whereby the
Fe-His
band appears at 225 cm
1.
The resonance Raman spectra of the HemAT-Bs(CO) with
12C16O and 13C16O in
the low frequency (300-700 cm
1) and high frequency
(1800-2100 cm
1) regions are shown in Fig.
6. The isotope shifts of 3, 19, and 46 cm
1 were observed for the bands at 494, 570, and 1964 cm
1, respectively, upon substitution of
13C16O for 12C16O.
Based on the frequencies of these bands and sizes of the isotope shifts, we assign the 494, 570, and 1964 cm
1 bands to the
Fe-CO stretching (
Fe-CO), the Fe-C-O bending, and the
C-O stretching (
C-O) modes, respectively.

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Fig. 6.
The isotope shift in the low and
high frequency resonance Raman spectra of HemAT-Bs(CO).
12C16O (a),
13C16O (b), and
12C16O-13C16O
(c) represent the Raman spectra of
HemAT-Bs(12C16O),
HemAT-Bs(13C16O), and HemAT-Bs
(12C16O)-HemAT-Bs(13C16O),
respectively.
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It is established that the
Fe-CO and
C-O
frequencies display an inverse linear correlation (53, 54) because of
the
-electron back donation mentioned above. This
-back donation
results in strengthening of the Fe-CO bond and concomitant weakening
of the C-O bond (or vice versa), leading to the empirical
Fe-CO versus
C-O linear
inverse line (53, 54). The
Fe-CO versus
C-O correlation depends on the nature of the proximal
ligand; the CO-bound hemes with an imidazole/histidine as the trans
ligand exhibit a correlation line different from those with a thiolate or imidazolate. The
Fe-CO and
C-O bands
of HemAT-Bs(CO), detected at 494 cm
1 and 1964 cm
1, respectively, fell on the imidazole/histidine
correlation curve as illustrated in Fig.
7. This fact means that proximal His is neutral like Mb, and the high frequency of the Fe-His stretching frequency cannot be ascribed to deprotonation of proximal His. The
Fe-CO and
C-O frequencies suggest that
the environment around the oxygen atom of bound CO is less hydrophilic
than that of native Mb like that in the open form of Mb. The negligibly
weak enhancement of the Fe-C-O bending band observed for
HemAT-Bs(CO), as shown in Fig. 6, suggests an undistorted
Fe-C-O geometry (54).

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Fig. 7.
Plot of
Fe-CO frequencies against
C-O frequencies observed for CO-bound
hemoproteins. Data obtained in the present study for HemAT-Bs are
shown by an open circle. Solid squares represent
data points of other CO adducts taken from Table II. Data for human Hb
A and Mb (pH 2.6 and 8.4) were from Ref. 49.
|
|
 |
DISCUSSION |
Structural Characteristics of Heme Pocket of HemAT-Bs--
The
Fe-O2 frequency of
HemAT-Bs(O2) in the 16O2 spectrum
(Fig. 4a, 560 cm
1) is one of the lowest
Fe-O2 stretching frequencies among O2-bound hemoproteins having a histidine as an axial ligand (33, 34, 47,
55-61). Recently, Yeh et al. (47) have reported a low
Fe-O2 stretching frequency (560 cm
1) for
hemoglobin from Mycobacterium tuberculosis (Mt
Hb). In conjunction with the mutagenesis studies, they have proposed a
unique hydrogen bonding pattern between the bound oxygen and the distal
tyrosine at the B10 position (the tenth residue in the B helix) through the sp2 orbital of the proximal oxygen atom and
have pointed out that this unique hydrogen bonding plays a crucial role
in the low frequency of the
Fe-O2 mode for Mt
Hb (47). Considering the low frequency of the
Fe-O2 mode of
HemAT-Bs(O2) comparable to that of Mt Hb, such a
unique hydrogen bonding as seen for Mt Hb would also be involved between one or more distal amino acid residues and the proximal oxygen atom of the bound O2 in
HemAT-Bs(O2). Specification of the hydrogen bonding
counterpart residue is under progress in this laboratory.
The important determinants of the
Fe-His frequency is
the hydrogen bonding status of the His N
hydrogen
(52), the strain imposed on the axial His by the protein moiety (62),
and geometry of bound imidazole (63). In practice, a high frequency
shift as large as 25 cm
1 was reported to be caused by
deprotonation of bound imidazole in imidazole-coordinated high spin
Fe(II) porphyrin (64). In cytochrome c peroxidase, the
strong hydrogen bond between the axial His and Asp235
enhances the anionic character of the imidazole ring of the axial His,
resulting in the higher
Fe-His frequency (245 cm
1) (65). When this hydrogen bond is disrupted by the
Asp235 to Asn mutation, the
Fe-His band is
shifted to a lower frequency (205 cm
1) (66, 67). Deoxy
Mb, which has a weak hydrogen bond on the axial His, gives the
Fe-His mode around 220 cm
1 (48). Thus,
deoxy HemAT-Bs may possibly have a stronger hydrogen bond compared with
deoxy Mb.
The effect of strain from the protein on the
Fe-His
frequency is most clearly seen for deoxy Hb, which gives different
Fe-His frequencies between the T (
Fe-His = 215 cm
1) and R (
Fe-His = 221 cm
1) structures (62). The low
Fe-His
frequency is a consequence of the strain in the T quaternary structure,
and the magnitude of strain is directly related to oxygen affinity
(68). In the absence of strain, the
Fe-His frequency is
close to that of deoxy Mb. The high
Fe-His frequency is
also observed for a cavity mutant of Mb (226 cm
1), in
which the axial His is replaced with Gly in the presence of exogenous
imidazole (69). In this case, an exogenous imidazole acts as the
proximal ligand, and the strain on the coordinated imidazole should be
absent. Such a cavity mutant was also be prepared for sGC (70),
heme-bound heme-oxygenase (71), and CooA (39), which show similar
phenomena. Accordingly, the higher vibrational frequency of the
Fe-His mode in deoxy HemAT-Bs is indicative of less
strain being imposed on the Fe-His bond compared with other
hemoproteins listed in Table IV except for Mt Hb.
Desbois and coworkers (63) investigated the geometry dependence of
Fe-His frequencies and found that
Fe-His
frequencies fall on a straight line with the inclination of
0.5
cm
1/deg when they are plotted against dihedral angles
(
) formed by the imidazole plane and the nearest
N(pyrrole)-Fe-N(pyrrole) axis. This correlation is different between
the imidazolate and imidazole groups, although both give higher
frequency for smaller
values. On the basis of this correlation,
Desbois and co-workers (63) interpreted the high
Fe-His
frequency (228-231 cm
1) of cytochrome c' in
terms of a large
angle for strongly hydrogen-bonded imidazole coordination.
Recently, Andrew et al. (72) observed a relatively high
Fe-His frequency (231 cm
1) for
Alcaligenes xylosoxidas cytochrome c'. According
to the x-ray structure of this protein in the oxidized form, the
angle is 33°, and accordingly, the high
Fe-His
frequency seemed to be due to deprotonation of proximal His. However,
the x-ray structure for the oxidized form did not exhibit a hydrogen
bonding counterpart of proximal His. Furthermore, the
Fe-CO versus
C-O correlation of this protein indicated the coordination of neutral imidazole at the
trans position of CO. Therefore, Andrew et al. assumed that
the structure in the proximity of heme changes with the oxidation state
of iron as well as upon ligand binding. Although the x-ray crystallographic structure is not available for HemAT, its
Fe-His frequency is too high to interpret it
in terms of a neutral imidazole coordination even for
= 0°,
but its
Fe-CO versus
C-O
correlation suggests the coordination of a neutral imidazole. Thus, the
same kind of dilemma as seen for A. xylosoxidas cytochrome
c' is present. Also in the case of HemAT-Bs, a structural
change would take place in the proximal side of the heme upon the
ligand binding, as is suggested for A. xylosoxidas
cytochrome c'. Such a conformational change in the proximal
heme pocket might be concerned with signal transduction in
HemAT-Bs.
Porphyrin Skeletal Vibrational Modes in the Low Frequency
Region--
In Table V, the low
frequency porphyrin skeletal modes of HemAT-Bs(O2),
HemAT-Bs(CO), and Mb are listed. The peak assignment was mainly based
on the study of Hu and co-workers (73).
The
8 mode, which has been reported to involve the
bending motions of peripheral substituents of porphyrin (74), is
believed to be sensitive to changes that occur in the distal side of
the heme pocket upon binding of a ligand (75). For the replacement of
O2 by CO, the largest shift of 11 cm
1 was
observed for the
8 mode of HemAT-Bs. The corresponding
frequency shift in Mb is 2 cm
1. This suggests that
binding of O2 to the heme of HemAT-Bs appreciably changes a
structure of the distal side of heme pocket through strong hydrogen
bonding to the bound oxygen but binding of CO does little.
Relation between Structure and Kinetic
Characteristics--
Resonance Raman spectroscopy of
HemAT-Bs(O2) has revealed that a distal amino acid residue
is hydrogen bonding to the proximal atom of bound oxygen molecule as
described above. Although Mt Hb (46) and Ascaris
Hb (77) have a hydrogen bonding network similar to that of HemAT-Bs,
they have an oxygen affinity very different from that of HemAT-Bs. The
difference in oxygen affinity is mainly due to very small
koff values for Mt Hb and
Ascaris Hb compared with that for HemAT-Bs (Table I),
whereas all have similar kon values except for
Ascaris Hb. Indeed, the koff value for HemAT-Bs(O2) is greater than those for Mt Hb
and Ascaris Hb by 100- and 5000-fold, respectively. We note
here that koff depends on the free energy of the
whole protein in the oxygenated form relative to that of the transient
state. When the strong hydrogen bond between the bound oxygen and
distal residues causes some strain in other parts of the protein, the
stabilization of the oxygenated form by the strong hydrogen bonds would
be partially canceled. Such a feature is really seen for deoxy Hb with
T structure, in which the inter-subunit hydrogen bonds are stronger and
free energy is lower in the T than R state, but the Fe-His bond is weaker in the T than R state due to the strain imposed on
the proximal His by the protein. In other words, the globin moiety is
stabilized whereas the heme group is destabilized by the hydrogen bonds
between subunits. The binding of a ligand to one heme of Hb is conveyed
to another heme via changes in the inter-subunit hydrogen bonds.
Accordingly, it is highly likely that HemAT-Bs utilizes a similar
character of protein for signal transduction and thus to work as an
O2 sensor.
It is interesting to note that Paramecium caudatum
(Pc) Hb exhibits similar kinetics and equilibrium parameters
for oxygen binding to those of HemAT-Bs (23). Although Pc Hb
possesses a distal E7 glutamine and a B10 tyrosine that form a hydrogen bond to the proximal and terminal oxygen atoms, respectively (23), it
gives a koff value (25.2 s
1)
larger than those for Mt Hb and Ascaris Hb but
close to that of HemAT-Bs (koff = 23 s
1). The
Fe-O2
mode of Pc Hb appears at 563 cm
1 (23), which
is similar to those of HemAT-Bs and Mt Hb (Table IV). Das
et al. (23) have proposed that the oxy complex of
Pc Hb is an equilibrium mixture of a hydrogen-bonded closed
structure and non-hydrogen bonded open structure and that oxygen will
dissociate preferentially from the open structure. Because the
Fe-O2 stretching Raman band of HemAT-Bs(O2) is
broad and likely to be composed of multiple bands as mentioned above,
we cannot rule out the possibility that there are two oxygenated forms
in HemAT-Bs(O2), that is, hydrogen-bonded and
non-hydrogen-bonded forms, and that oxygen is dissociated from the latter.
HemAT-Bs(O2) shows an autoxidation rate significantly
slower than those of LegHb and FixL as shown in Table II. The
autoxidation rate of HemAT-Bs(O2) is close to that of Mb.
It is well known that the bound O2 of Mb is stabilized by a
hydrogen bond from the distal His, and accordingly, the bound
O2 of HemAT-Bs would be stabilized to a similar extent. An
extremely small autoxidation rate constant for Mt Hb is
probably caused by hydrogen bonding to the proximal oxygen atom within
a closed distal heme pocket (26). The increased autoxidation rate of
HemAT-Bs compared with Mt Hb, despite the strong hydrogen
bonding to the proximal oxygen atom similar to that in Mt
Hb, might be due to the presence of the second conformer with a
relatively open distal heme pocket.
Primary Structure of HemAT-Bs--
It has been reported that the
N-terminal region of HemAT-Bs and HemAT-Hs exhibit an amino acid
sequence homology to Mb (9). Alignment of the heme binding domain of
HemAT-Bs (10) with some globin sequences is shown in Fig.
8. Among these proteins, the proximal
histidine at the F8 position is conserved, but amino acid residues at
the B10 and E7 positions are not. It has been recently confirmed that
His123 corresponding to a histidine at the F8 position does
indeed act as the proximal ligand of the heme in HemAT-Bs (10). A
tyrosine at the B10 position in Mt Hb and Pc Hb
hydrogen bonds to the bound oxygen (23, 47). In HemAT-Bs, however, the
residue at the B10 position would be a leucine, an amino acid not
capable of hydrogen bonding, as is the case for Sw Mb. The
distal residue at the E7 position in Sw Mb and Pc
Hb, His64 and Gln42, respectively, also
hydrogen bonds to the bound oxygen (23, 78). In HemAT-Bs, the residue
at the E7 position would be a serine, Ser87. Although a
serine is a possible candidate for an amino acid residue hydrogen
bonding to the bound oxygen, there is not any direct evidence at
present that the Ser87 is involved in the hydrogen bonding
network in HemAT-Bs(O2).

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Fig. 8.
Alignment of the heme-binding domain of
HemAT-Bs with some globin sequences. The distal positions at B10
and E7, and the proximal histidine at F8 position are indicated.
Abbreviations used are: Sw Mb, sperm whale myoglobin;
Mt Hb, M. tuberculosis hemoglobin;
Pc Hb, P. caudatum hemoglobin.
|
|
In a preliminary resonance Raman study of S87A HemAT-Bs, in
which Ser87 is replaced by Ala, the
Fe-O2 mode was observed at
563 cm
1. In the case of Chlamydomonas
eugametos Hb, the mutation of the B10 Tyr or E7 Gln, both of which
hydrogen bond to the bound oxygen, results in the up-shift of the
Fe-O2 mode by 7 or 15 cm
1, respectively (79). Compared with the case for
C. eugametos Hb, the
Fe-O2 mode is not perturbed
as much by the mutation of Ser87 to Ala in the case of
HemAT-Bs. Thus we need additional experiments to find out if
Ser87 hydrogen bonds to the bound oxygen and to determine
the distal amino acid residue that hydrogen bonds to the bound oxygen.
Oxygen Sensing and Signal Transduction Mechanisms for
HemAT-Bs--
A conformational change induced by the ligand binding to
the heme is a crucial step for the effector sensing and signal
transduction in the heme-based sensor proteins. For the CO sensor
protein CooA, CO replaces one of the endogenous axial ligands,
Pro2, upon the binding to the six-coordinated ferrous heme,
which results in a conformational change in the N-terminal region
and/or in a relocation of the heme with a conformational change of the proximal heme pocket (39, 80, 81). The ligand exchange between Pro2 and CO is the first step of the CO sensing in the case
of CooA. This sensing mechanism would be specific for CooA among CooA, FixL, and HemAT-Bs, because only the heme in CooA is six-coordinate in
the resting state (20, 80). FixL and HemAT-Bs contain a five-coordinate
heme in their resting state, and oxygen binds to a vacant distal site
of the heme.
In the case of FixL, the sensing mechanism is completely different from
that for CooA. Gong et al. (82) have reported that oxygen
binding to the heme in FixL induces rearrangements of the hydrogen
bonding network between the heme 6- and 7-propionates and amino acid
residues (Arg206 and His214) in the F/G loop
region that results in the flattening of the heme plane upon the ligand
binding. They propose that the signal transduction might be mainly
driven by the motion of the heme plane induced by oxygen binding (82).
On the other hand, Mukai et al. (83) have proposed that the
interaction between Ile209 (and/or Ile210),
which are located on the F/G loop region, and the iron-bound oxygen is
essential for oxygen sensing by FixL.
Although both of FixL and HemAT-Bs are oxygen sensor proteins, they
show no structural homology. HemAT-Bs is a member of globin-coupled sensor proteins (10), whereas FixL is a member of the PAS domain superfamily (84). Furthermore, oxygen binding and autoxidation kinetics
are completely different between FixL and HemAT-Bs, as described in
this work. These results suggest that the oxygen-sensing mechanism for
HemAT-Bs will be different from that for FixL.
Oxygen binding to the heme iron in Hb results in a movement of the iron
ion into the heme plane along with the movement of the proximal
histidine and F helix, which is a trigger of the allosteric control for
Hb. As described in this work, HemAT-Bs shows amino acid sequence
homology and similar spectroscopic and ligand binding properties to
those of Mbs and Hbs. These results suggest that a similar
conformational change, i.e. a movement of the heme iron with
the proximal ligand and F helix, upon the oxygen binding could be a
trigger of the signal transduction for HemAT-Bs. Given that this is the
case, however, CO should have the same effect as O2.
Because CO is not a physiological effector of HemAT-Bs, HemAT-Bs should
discriminate between O2 and CO. Hydrogen bonding to the
bound oxygen is considered to play a crucial role for the ligand
discrimination as discussed above, but further studies are required to
determine if this is the case.
 |
ACKNOWLEDGEMENTS |
We thank Professors I. Okura and T. Kamachi
of Tokyo Institute of Technology for help in laser flash photolysis experiments.
 |
FOOTNOTES |
*
This work was supported by a Grant-in-Aid for Scientific
Research of Priority Areas on Metal Sensors 12147203 and by 12680631 (to S. A.), 12740361 (to H. N.), and 12045264 (to T. K.) from the
Ministry of Education, Culture, Sports, Science, and Technology of
Japan.The costs of publication of this
article were defrayed in part by the
payment of page charges. The article
must therefore be hereby marked
"advertisement" in
accordance with 18 U.S.C. Section
1734 solely to indicate this fact.
§
To whom correspondence may be addressed: Tel.: 81-761-51-1681; Fax:
81-761-51-1149; E-mail: aono@jaist.ac.jp.
To whom correspondence may be addressed: Tel.: 81-564-55-7340;
Fax: 81-564-55-4639; E-mail: teizo@ims.ac.jp.
Published, JBC Papers in Press, January 30, 2002, DOI 10.1074/jbc.M112256200
 |
ABBREVIATIONS |
The abbreviations used are:
MCP, methyl-accepting chemotaxis protein;
HemAT-Bs, HemAT from B. subtilis;
HemAT-Hs, HemAT from H. salinarum;
HemAT-Bs(O2), the oxy form of HemAT-Bs;
HemAT-Bs(CO), the
CO-bound form of HemAT-Bs;
sGC, soluble guanylate cyclase;
Mb, myoglobin;
Hb, hemoglobin;
Mb(CO), the CO-bound form of myoglobin;
FixL(O2), the oxygen-bound form of FixL.
 |
REFERENCES |
| 1.
|
Parkinson, J. S.
(1993)
Cell
73,
857-871[CrossRef][Medline]
[Order article via Infotrieve]
|
| 2.
|
Hoff, W. D.,
Jung, K.-H.,
and Spudich, J. L.
(1997)
Annu. Rev. Biophys. Biomol. Struct.
26,
223-258[CrossRef][Medline]
[Order article via Infotrieve]
|
| 3.
|
Stock, J. B.,
and Lukat, G. S.
(1991)
Annu. Rev. Biophys. Biophys. Chem.
20,
109-136[CrossRef][Medline]
[Order article via Infotrieve]
|
| 4.
|
Parkinson, J. S.,
and Kofoid, E. C.
(1992)
Annu. Rev. Genet.
26,
71-112[CrossRef][Medline]
[Order article via Infotrieve]
|
| 5.
|
Garrity, L. F.,
and Ordal, G. W.
(1995)
Pharmacol. Ther.
68,
87-104[CrossRef][Medline]
[Order article via Infotrieve]
|
| 6.
|
Blair, D. F.
(1995)
Annu. Rev. Microbiol.
49,
489-522[CrossRef][Medline]
[Order article via Infotrieve]
|
| 7.
|
Hazelbauer, G. L.
(1992)
Curr. Opin. Struct. Biol.
2,
505-510[CrossRef]
|
| 8.
|
Falke, J. J.,
and Hazelbauer, G. L.
(2001)
Trends Biochem. Sci.
26,
257-265[CrossRef][Medline]
[Order article via Infotrieve]
|
| 9.
|
Hou, S.,
Larsen, R. W.,
Boudko, D.,
Riley, C. W.,
Karatan, E.,
Zimmer, M.,
Ordal, G. W.,
and Alam, M.
(2000)
Nature
403,
540-544[CrossRef][Medline]
[Order article via Infotrieve]
|
| 10.
|
Hou, S.,
Freitas, T.,
Larsen, R. W.,
Piatibratov, M.,
Sivozhelezov, V.,
Yamamoto, A.,
Meleshkevithch, E. A.,
Zimmer, M.,
Ordal, G. W.,
and Alam, M.
(2001)
Proc. Natl. Acad. Sci. U. S. A.
98,
9353-9358[Abstract/Free Full Text]
|
| 11.
|
Rodgers, K. R.
(1999)
Curr. Opin. Chem. Biol.
3,
158-167[CrossRef][Medline]
[Order article via Infotrieve]
|
| 12.
|
Aono, S.,
and Nakajima, H.
(1999)
Coord. Chem. Rev.
190-192,
267-282[CrossRef]
|
| 13.
|
Aono, S.,
and Nakajima, H.
(2000)
Prog. React. Kinet. Mech.
25,
65-107
|
| 14.
|
Chan, M. K.
(2001)
Curr. Opin. Chem. Biol.
5,
216-222[CrossRef][Medline]
[Order article via Infotrieve]
|
| 15.
|
Gilles-Gonzalez, M. A.,
Ditta, G. S.,
and Helinski, D. R.
(1991)
Nature
350,
170-172[CrossRef][Medline]
[Order article via Infotrieve]
|
| 16.
|
Delgado-Nixon, V. M.,
Gonzalez, G.,
and Gilles-Gonzalez, M. A.
(2000)
Biochemistry
39,
2685-2691[CrossRef][Medline]
[Order article via Infotrieve]
|
| 17.
|
Chang, A. L.,
Tuckerman, J. R.,
Gonzalez, G.,
Mayer, R.,
Weinhouse, H.,
Volman, G.,
Amikam, D.,
Benziman, M.,
and Gilles-Gonzalez, M. A.
(2001)
Biochemistry
40,
3420-3426[CrossRef][Medline]
[Order article via Infotrieve]
|
| 18.
|
Denninger, J. W.,
and Marletta, M. A.
(1999)
Biochim. Biophys. Acta
1411,
334-350[Medline]
[Order article via Infotrieve]
|
| 19.
|
Aono, S.,
Nakajima, H.,
Saito, K.,
and Okada, M.
(1996)
Biochem. Biophys. Res. Commun.
228,
752-756[CrossRef][Medline]
[Order article via Infotrieve]
|
| 20.
|
Aono, S.,
Ohkubo, K.,
Matsuo, T.,
and Nakajima, H.
(1998)
J. Biol. Chem.
273,
25757-25764[Abstract/Free Full Text]
|
| 21.
|
Shelver, D.,
Kerby, R. L., He, Y.,
and Roberts, G. P.
(1997)
Proc. Natl. Acad. Sci. U. S. A.
94,
11216-11220[Abstract/Free Full Text]
|
| 22.
|
Kiger, L.,
Rashid, A. K.,
Griffon, N.,
Haque, M.,
Moens, L.,
Gibson, Q. H.,
Poyart, C.,
and Marden, M. C.
(1998)
Biophys. J.
75,
990-998[Abstract/Free Full Te |