|
|
||||||||
| ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
Department of Physiology, University of Tennessee Health Science Center, Memphis, Tennessee
Submitted 21 November 2005 ; accepted in final form 17 January 2006
| ABSTRACT |
|---|
|
|
|---|
55% of control in cav-1+/+ cells but did not alter transient KCa current frequency in cav-1/ cells. Furthermore, although KCa channel density was elevated in cav-1/ cells, transient KCa current amplitude was similar to that in cav-1+/+ cells. Higher Ca2+ spark frequency in cav-1/ cells was not due to elevated intracellular Ca2+ concentration, sarcoplasmic reticulum Ca2+ load, or nitric oxide synthase activity. Similarly, Ca2+ spark amplitude and spread, the percentage of Ca2+ sparks that activated a transient KCa current, the amplitude relationship between sparks and transient KCa currents, and KCa channel conductance and apparent Ca2+ sensitivity were similar in cav-1+/+ and cav-1/ cells. In summary, cav-1 ablation elevates Ca2+ spark and transient KCa current frequency, attenuates the coupling relationship between voltage-dependent Ca2+ channels and RyR channels that generate Ca2+ sparks, and elevates KCa channel density but does not alter transient KCa current activation by Ca2+ sparks. These findings indicate that cav-1 is required for physiological Ca2+ spark and transient KCa current regulation in cerebral artery smooth muscle cells.
ryanodine-sensitive Ca2+ release channel; large-conductance Ca2+-activated potassium channel; caveolae; voltage-dependent Ca2+ channel
Smooth muscle cells generate several different modes of Ca2+ signaling (15, 20). The global intracellular Ca2+ concentration ([Ca2+]i) arises because of extracellular Ca2+ influx and intracellular Ca2+ release. An elevation in global [Ca2+]i stimulates contraction, whereas a reduction in global [Ca2+]i results in relaxation. Localized [Ca2+]i transients, termed "Ca2+ sparks," also occur in smooth muscle cells (20, 27). Ca2+ sparks occur due to the opening of several ryanodine-sensitive Ca2+ release (RyR) channels on the sarcoplasmic reticulum (SR) (15, 27). In smooth muscle cells, a Ca2+ spark does not directly elevate global Ca2+ but activates a number of nearby large-conductance Ca2+-activated potassium (KCa) channels, resulting in a transient KCa current. Membrane hyperpolarization induced by asynchronous transient KCa currents reduces voltage-dependent Ca2+ channel activity, leading to a decrease in global [Ca2+]i and relaxation. An elevation in [Ca2+]i activates Ca2+ sparks and transient KCa currents, forming a negative-feedback loop that limits Ca2+ entry through voltage-dependent Ca2+ channels (15, 27). Thus voltage-dependent Ca2+ channels, RyR channels, and KCa channels comprise a functional unit that regulates smooth muscle contractility (17). The differential regulation of contractility by local and global Ca2+ signaling is also effective because of differences in the frequency and amplitude of the Ca2+ signals and the Ca2+ sensitivities of the downstream targets for each signal mode (15). For local Ca2+ signaling mechanisms to operate, downstream targets must also be located in the proximity of the Ca2+ source. In smooth muscle cells, whether membrane proteins maintain spatial organization of voltage-dependent Ca2+ channels, KCa channels, and RyR channels to permit Ca2+ signaling between these proteins is unclear.
Compartmentalization of signaling molecules can occur in small, cholesterol-enriched, flask-shaped membrane invaginations termed "caveolae" (11, 13, 34, 39). Caveolins, of which three isoforms have been cloned (cav 13), are structural components required for caveolae formation (11, 13, 34, 39). Although all three caveolins have been identified in vascular smooth muscle cells, caveolin-1 is the primary isoform (9, 18, 28, 34, 39). Supporting a role for caveolae in the regulation of arterial smooth muscle local Ca2+ signaling is evidence that acute cholesterol depletion with dextrin inhibits Ca2+ sparks (23). Similarly, transient KCa current frequency is reduced in cerebral artery smooth muscle cells of cav-1-deficient (cav-1/) mice, when compared with wild-type controls (10). In ureter smooth muscle cells, KCa channels are found in buoyant membrane fractions, and in cultured myometrial cells KCa channels are localized to caveolae (1, 3). Thus cav-1 and caveolae may regulate Ca2+ sparks and KCa channels in smooth muscle.
Here, the communication between voltage-dependent Ca2+ channels and RyR channels that generate Ca2+ sparks and signaling between Ca2+ sparks and KCa channels was investigated in cerebral artery smooth muscle cells of cav-1+/+ and cav-1/ mice. Data indicate that cav-1 ablation abolishes caveolae, elevates Ca2+ spark frequency, and attenuates Ca2+ spark regulation by voltage-dependent Ca2+ channels. In contrast, transient KCa current activation by Ca2+ sparks is unaltered in cav-1/ cells, even though there is an increase in KCa channel density.
| MATERIALS AND METHODS |
|---|
|
|
|---|
150 µm in diameter) were removed, cleaned of connective tissue, and maintained in ice-cold Ca2+-free buffer (solution A) containing (in mM) 55 NaCl, 80 Na glutamate, 5.6 KCl, 2 MgCl2, 10 HEPES, and 10 glucose (pH 7.3 with NaOH). For single cell isolation, smooth muscle cells were dissociated from cerebral arteries with the use of enzymes, as previously described (14). Electron microscopy. The brain was fixed in PSS containing 2.5% glutaraldehyde for 1 h. Cerebral arteries were dissected from the fixed brain, cleaned of connective tissue, and postfixed in 1% osmium tetroxide in PSS for 4 h. Arteries were then rinsed briefly in deionized water and en bloc stained with 2% uranyl acetate in 0.85% sodium chloride overnight at 4°C. Arteries were dehydrated in graded solutions of ethanol, from 30% through 100% for 1 h each, infiltrated with 50% Spurr in 100% ethanol overnight at room temperature, 100% Spurr over an 8-h period involving at least three changes of Spurr, and then cured at 60°C for 2 days. Transverse sections (75 nm) were cut with a Reichert Ultracut E microtome and poststained with uranyl acetate and lead citrate. Cells were observed and photographed with a JEOL 2000EX TEM located in the Electron Microscope Facility at the University of Tennessee Health Science Center.
Patch-clamp electrophysiology.
Potassium currents were measured by using the conventional whole cell, perforated-patch or inside-out patch-clamp configurations with an Axopatch 200B amplifier and Clampex 8.2 (Axon Instruments, Union City, CA). For transient KCa current measurement, the bath solution (solution B) contained (in mM) 134 NaCl, 6 KCl, 2 CaCl2, 1 MgCl2, 10 HEPES, and 10 glucose (pH 7.4 with NaOH), and the pipette solution contained (in mM) 110 potassium aspartate, 30 KCl, 10 NaCl, 1 MgCl2, 10 HEPES, and 0.05 EGTA (pH 7.2 with KOH). Amphotericin B (Sigma) was dissolved in DMSO and diluted into the pipette solution to give a final concentration of 200 µg/ml. For whole cell K+ current measurement, the bath solution was solution B and the pipette solution contained (in mM) 135 KCl, 5 EGTA, 1.0 BAPTA, 3.5 MgCl2, 2.5 Na2ATP, and 10 HEPES (pH 7.2 with KOH). For inside-out patch-clamp experiments to measure single KCa channel currents, the pipette and bath solution both contained (in mM) 140 KCl, 10 HEPES, 5 EGTA, and 1.6 1-N-(2-hydroxyethyl)ethylenediamine-N,N',N'-triacetic acid (pH 7.2 with KOH). MgCl2 and CaCl2 were supplemented to bath solution to provide 1 mM free Mg2+ and the required free Ca2+ concentration (1100 µM). Free Ca2+ concentration in the pipette solution was 10 µM. Free Ca2+ concentrations were measured by using a Ca2+-sensitive and reference electrode (Corning). For voltage-dependent Ba2+ current measurements, the pipette solution contained (in mM) 125 CsCl, 20 tetraethylammonium chloride (TEACl), 1.0 MgCl2, 0.5 EGTA, 10 HEPES, and 10 glucose (pH 7.2 with CsOH), and the bath solution contained (in mM) 60 NaCl, 60 TEACl, 1.0 MgCl2, 20 BaCl2, 10 glucose, and 10 HEPES (pH 7.4 with NaOH). Pipette resistance was measured by applying a 5-mV pulse using the seal test function of pClamp 8.2. Transient KCa currents were measured at a steady membrane potential of 40 mV. Voltage-dependent Ba2+ currents were activated from a holding potential of 80 mV by applying 300-ms voltage steps to voltages between 50 and +60 mV in increments of 10 mV. Whole cell K+ (Ik) currents were activated from a holding potential of 80 mV by applying 250-ms voltage steps to voltages between 70 and +80 mV in 10-mV increments. In inside-out patches, single KCa channel currents were measured at steady voltages of 40 or +40 mV. Transient KCa currents were filtered at 1 kHz and digitized at 5 kHz. Voltage-dependent Ba2+ currents were filtered at 1 kHz and digitized at 4 kHz. Other current measurements were filtered at 2 kHz and digitized at 10 kHz. Transient KCa current analysis was performed off-line using methodology described elsewhere (6). A transient KCa current was defined as the simultaneous opening of three or more KCa channels. Open probability (Po) was calculated from the following equation: Po = (
tii)/nT, where ti is the time at each channel level i, n is the number of channels in the patch, and T is the total time of analysis. The total number of KCa channels in an inside-out patch was determined at a voltage of +40 mV with 100 µM free Ca2+ in the bath solution. In each patch under each condition, at least 5 min of continuous data were analyzed to calculate transient KCa current frequency and amplitude, and 25 min were analyzed to determine single KCa channel open probability.
Confocal Ca2+ imaging. Isolated smooth muscle cells were incubated in solution A containing fluo-4 AM (10 µM) for 20 min at room temperature, followed by a 30-min wash to allow indicator deesterification. Smooth muscle cells were imaged with the use of a Noran Oz laser scanning confocal microscope (Noran Instruments, Middleton, WI) and a x60 water immersion objective (1.2 numerical aperture) attached to a Nikon TE300 microscope. Fluo-4 was excited by using the 488 nm line of a krypton-argon laser, and emitted light >500 nm was captured. Images (56.3 x 52.8 µm) were recorded every 8.3 ms (120 images/s). The laser intensity used did not alter transient KCa current frequency or amplitude. Current and fluorescence measurements were synchronized by using a light-emitting diode placed above the recording chamber that was triggered during acquisition. Each cell was imaged for 15 s. Ca2+ sparks in smooth muscle cells were analyzed with the use of software kindly provided by Dr. M. T. Nelson (University of Vermont). Detection of Ca2+ sparks was performed by dividing an area 1.54 µm (7 pixels) x 1.54 µm (7 pixels) (i.e., 2.37 µm2) in each image (F) by a baseline (F0) that was determined by averaging 10 images without Ca2+ spark activity. The entire area of each image was analyzed to detect Ca2+ sparks. A Ca2+ spark was defined as a local increase in F/F0 that was >1.2.
Fura-2 imaging.
Cerebral arteries were incubated with the ratiometric fluorescent Ca2+ indicator fura-2 AM (5 µM) and 0.05% pluronic F-127 for 20 min, followed by a 15-min wash. All experiments were performed using solution B (composition described in Patch-clamp electrophysiology). Fura-2 was alternately excited at 340 or 380 nm using a PC-driven hyperswitch (Ionoptix, Milton, MA). Background corrected ratios were collected every 1 s at 510 nm using a photomultiplier tube (Ionoptix). SR Ca2+ load ([Ca2+]SR) was estimated by rapidly applying a high concentration of caffeine (10 mM), an RyR channel activator, and measuring the amplitude of [Ca2+]i transients (i.e.,
[Ca2+]i). Intracellular Ca2+ concentrations were calculated by using the following equation (12):
![]() |
Measurement of cellular dimensions. Isolated smooth muscle cells were allowed to settle on a glass coverslip in a chamber with Ca2+-free, HEPES-containing patch-clamp bath solution (composition described in Patch-clamp electrophysiology). Cell images were acquired with the use of a Zeiss LSM5 confocal microscope. Cell length and width were calculated using Pascal software (Zeiss).
Statistics. Values are expressed as means ± SE. Student's t-test and Student-Newman-Keuls test were used for comparing paired or unpaired data and multiple data sets, respectively. Simultaneous Ca2+ spark and transient KCa current amplitude data were fit with a linear regression function, and the slope ± SE of each fit was compared using Students t-test and Graphpad Prizm (San Diego, CA). P < 0.05 was considered significant.
| RESULTS |
|---|
|
|
|---|
150 µm) cerebral arteries of cav-1+/+ mice (Fig. 1, A and B). In contrast, caveolae were not observed in cerebral artery smooth muscle cells of cav-1/ mice (Fig. 1, C and D). These data indicate that cav-1 is necessary for caveolae formation in smooth muscle cells of small cerebral arteries.
|
|
8.4 pF) was smaller than for cav-1+/+ cells (
12.1 pF; Fig. 2D). To investigate whether cell size underlies the difference in cav-1+/+ and cav-1/ cell capacitance, cellular dimensions were measured. Cells were observed in a Ca2+-free bath solution to induce maximal relaxation. Cav-1+/+ and cav-1/ cell length [in µm: cav-1+/+, 37.1 ± 1.6 (n = 32); cav-1/, 39.4 ± 2.6 (n = 33)] and width [in µm: cav-1+/+, 9.6 ± 0.3 (n = 32); cav-1/, 9.4 ± 0.3 (n = 33)] were not different (P > 0.05 for each). These data suggest that cav-1 ablation reduces the cell surface area but does not alter the dimensions of cerebral artery smooth muscle cells. In arterial smooth muscle cells, transient KCa currents occur due to SR Ca2+ release (38). We sought to determine mechanisms that activate transient KCa currents in cav-1/ cells. In cav-1/ cells, thapsigargin (100 nM), an SR Ca2+ ATPase inhibitor, abolished transient KCa currents, indicating that these events occur due to SR Ca2+ release (Fig. 2E; n = 4).
Ca2+ spark frequency is elevated in cav-1/ cells when compared with cav-1+/+ cells, but the amplitude relationship between Ca2+ sparks and transient KCa currents is similar. Elevated transient KCa current frequency in cav-1/ cells could occur because of an increase in Ca2+ spark frequency or an increase in the percentage of Ca2+ sparks that activate a transient KCa current (i.e., percent coupling). To investigate these possibilities and to compare Ca2+ spark properties in cav-1+/+ and cav-1/ cells, simultaneous measurements of Ca2+ sparks and evoked transient KCa currents were obtained by performing confocal Ca2+ imaging in combination with patch-clamp electrophysiology.
At 40 mV, Ca2+ spark frequency was
1.8-fold higher in cav-1/ cells than in cav-1+/+ cells (Fig. 3, A and B). In contrast, Ca2+ spark amplitude (Fig. 3C) and spatial spread [full width at half-maximal amplitude; cav-1+/+, 1.82 ± 0.13 µm (n = 40); cav-1/, 1.94 ± 0.11 µm (n = 59)] were similar in cav-1+/+ and cav-1/ cells (P > 0.05 for each). The percentage of Ca2+ sparks that activated a transient KCa current (cav-1+/+, 67 ± 8%; cav-1/, 71 ± 4%) and the amplitude relationship between Ca2+ sparks and transient KCa currents were also similar (Fig. 3, A and D). Taken together, these data indicate that genetic ablation of cav-1/ elevates Ca2+ spark frequency, leading to an increase in transient KCa current frequency.
|
|
-nitro-L-arginine does not inhibit transient KCa currents in cav-1+/+ or cav-1/ cells.
Cav-1 ablation leads to nitric oxide (NO) synthase (NOS) activation and an increase in NO generation (10, 34). NO donors activate Ca2+ sparks in arterial smooth muscle cells (31). Therefore, we investigated whether Ca2+ spark frequency is higher in cav-1/ cells because of elevated NOS activity. N
-nitro-L-arginine (1 mM), a NOS blocker, did not alter transient KCa current frequency or amplitude in either cav-1+/+ [%control; frequency, 122 ± 16; amplitude, 107 ± 21 (n = 6)] or cav-1/ [frequency, 106 ± 13; amplitude, 90 ± 17 (n = 5)] cells (P > 0.05 for each). These data suggest that the Ca2+ spark frequency elevation in cav-1/ cells does not occur through NOS activation.
Transient KCa current regulation by voltage-dependent Ca2+ channels is abolished in cav-1/ cells.
In smooth muscle cells, Ca2+ sparks are activated by Ca2+ entering through sarcolemma voltage-dependent Ca2+ channels (14, 16, 20). We investigated whether Ca2+ sparks are more frequent in cav-1/ cells because of enhanced coupling between voltage-dependent Ca2+ channels and RyR channels. In cav-1+/+ cells, Cd2+ (250 µM), a voltage-dependent Ca2+ channel blocker, or diltiazem (50 µM), an L-type Ca2+ channel blocker, reduced transient KCa current frequency to
51 and
57% of control, respectively, but did not alter transient KCa current amplitude (Fig. 5, AC). In contrast, Cd2+ and diltiazem did not alter transient KCa current frequency or amplitude in cav-1/ cells (Fig. 5, AC). Thus Ca2+ spark regulation by voltage-dependent Ca2+ channels is abolished in cav-1/ cells, indicating that higher Ca2+ spark frequency is not through enhanced coupling between voltage-dependent Ca2+ channels and RyR channels.
|
|
Transient KCa current amplitude is dependent on KCa channel conductance and Ca2+ sensitivity (4). In excised inside-out patches, single KCa channel slope conductance between 40 and +40 mV [cav-1+/+, 268 ± 3 pS (n = 9); cav-1/, 260 ± 3 pS (n = 7); P > 0.05] and KCa channel-apparent Ca2+ sensitivity were similar in cav-1+/+ and cav-1/ cells (Fig. 7, A and B). Transient KCa current amplitude also depends on the number of KCa channels activated by a Ca2+ spark. On average, inside-out patches pulled from cav-1/ cells contained
1.5-fold more KCa channels than patches obtained from cav-1+/+ cells (Fig. 7C). This finding was not due to differences in the size of patch pipettes used for these experiments [cav-1+/+, 28.6 ± 1.2 M
(n = 17); cav-1/, 27.1 ± 0.7 M
(n = 22); P > 0.05]. These data suggest that sarcolemma KCa channel density is higher in cav-1/ cells than in cav-1+/+ cells.
|
|
| DISCUSSION |
|---|
|
|
|---|
In smooth muscle cells, coupling between voltage-dependent Ca2+ channels and RyR channels is "loose" (20). Although structural and molecular mechanisms that establish this coupling process are unclear, loss of voltage-dependent Ca2+ channel to RyR channel communication in cav-1/ cells likely occurs because of spatial separation of these proteins. Supporting this hypothesis is evidence that although voltage-dependent Ca2+ current density was similar in cav-1+/+ and cav-1/ cells, regulation of transient KCa currents by voltage-dependent Ca2+ channel blockers was abolished in cav-1/ cells. In addition, although KCa channel density was elevated in cav-1/ cells, mean transient KCa current amplitude was similar to that in cav-1+/+ cells. KCa channel conductance, Ca2+ spark amplitude and spatial spread, the effective coupling of Ca2+ sparks to KCa channels, and KCa channel-apparent Ca2+ sensitivity were similar in cav-1+/+ and cav-1/ cells. Caveolae are structural membrane invaginations that may reduce the sarcolemma to SR distance and physically localize RyR channels nearby voltage-dependent Ca2+ channels and KCa channels in cav-1+/+ cells. A flattening of the sarcolemma in cav-1/ cells may explain the proposed increase in the signaling distance between RyR channels and voltage-dependent Ca2+ channels and KCa channels. In cav-1/ cells, a distant spark would impact a smaller membrane area and induce a lower subsarcolemmal [Ca2+]i elevation. Consistent with our observations, higher KCa channel density would be required for distant Ca2+ sparks to activate transient KCa currents of similar amplitude to those in cav-1+/+ cells.
Another explanation for the proposed increase in signaling distance is that cav-1 abolishment leads to delocalization of voltage-dependent Ca2+ channels and KCa channels from within the vicinity of the spark site. Several lines of evidence support such a proposal. In smooth muscle cells, caveolae compartmentalize voltage-dependent Ca2+ channels and KCa channels (3, 8). In arterial smooth muscle cells, KCa channels are proposed not to cluster above Ca2+ sparks sites, although in Bufo marinus stomach smooth muscle cells, such clustering may occur (30, 42). In guinea pig bladder smooth muscle, peripheral SR and caveolae are in close proximity, and L-type Ca2+ channels located in caveolae strips may be closely opposed to SR RyR channels (25). It is not clear what causes the elevation in KCa channel density in cav-1/ cells, but in cultured human myometrial smooth muscle cells, KCa channels associate with caveolins 1 and 2, and cholesterol depletion with cyclodextrin leads to an increase in whole cell KCa current density (3), consistent with the results here. Furthermore, in bovine endothelial cells, cav-1 physically interacts with and inhibits KCa channels and this effect can be removed by cholesterol depletion, leading to channel activation (37).
Investigating the effects of chronic caveolae deficiency on smooth muscle Ca2+ signaling can provide insights into physiological regulation by these membrane organelles in cav-1+/+ cells and potential changes that occur during pathophysiology and ontogeny (11, 29, 32, 34, 39). In contrast to the observations here, acute cholesterol depletion with dextrin inhibited arterial smooth muscle Ca2+ sparks (23). Acute cholesterol depletion and chronic cav-1 ablation may differentially regulate Ca2+ spark frequency through opposing effects on signaling pathways that regulate these events, and in the case of the genetic model, through developmental changes that occur in the sustained absence of cav-1 (10, 39). However, dextrin treatment also induces a change in membrane fluidity that may inhibit Ca2+ sparks (26). In agreement, both dextrin and cav-1 ablation abolished coupling between voltage-dependent Ca2+ channels and RyR channels that generate sparks (present data and Ref. 23). Whereas dextrin treatment disrupts both caveolar and noncaveolar lipid rafts, in the absence of cav-1, noncaveolar lipid rafts would remain (see Ref. 40). Thus our data suggest that caveolae-localized voltage-dependent Ca2+ channels regulate Ca2+ sparks in arterial smooth muscle cells. In another previous study, transient KCa current frequency was reduced in arterial smooth muscle cells of cav-1/ mice (10). It is unclear why data here are contradictory to those observations, but in the previous study, effects of cav-1 deficiency on Ca2+ sparks were not measured (10).
Through its amino-terminal scaffolding domain, cav-1 inhibits the activity of many binding partners, including NOS, protein kinase C, and adenylyl cyclase (28, 34). Cav-1 is found in the cytosol (22) and, conceivably, may interact with and inhibit RyR channels. Cav-1 is also found in mitochondria, which regulate Ca2+ sparks in cerebral artery smooth muscle cells (7, 41). Cav-1 abolishment may also activate RyR channels indirectly by modulating the activity of signaling pathways that regulate Ca2+ sparks (e.g., see Refs. 15 and 41). Data here indicate that cav-1 ablation does not activate Ca2+ sparks through NOS activation (31, 33). Because cav-1 ablation may activate RyR channels directly and indirectly, future studies will be required to determine the specific underlying mechanisms. The physiological impact of the transient KCa current frequency elevation in cav-1/ cells would be a membrane hyperpolarization that reduces voltage-dependent Ca2+ channel activity, leading to a decrease in global [Ca2+]i and vasodilation (15). Cav-1/ aortas contract less in response to vasoconstrictors and relax more in response to acetylcholine, a vasodilator, when compared with cav-1+/+ arteries (10, 33), supporting upregulation of a vasodilatory pathway.
In summary, data show that genetic ablation of cav-1 leads to loss of caveolae, an increase in Ca2+ spark frequency, abolishment of Ca2+ spark regulation by voltage-dependent Ca2+ channels, and an increase in KCa channel density in cerebral artery smooth muscle cells. In contrast, cav-1 ablation does not attenuate transient KCa current activation by Ca2+ sparks.
| GRANTS |
|---|
|
|
|---|
| ACKNOWLEDGMENTS |
|---|
| FOOTNOTES |
|---|
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.
| REFERENCES |
|---|
|
|
|---|
1 subunit of the calcium-activated potassium channel. Nature 407: 870876, 2000.[CrossRef][Medline]This article has been cited by other articles:
![]() |
S. A. Predescu, D. N. Predescu, and A. B. Malik Molecular determinants of endothelial transcytosis and their role in endothelial permeability Am J Physiol Lung Cell Mol Physiol, October 1, 2007; 293(4): L823 - L842. [Abstract] [Full Text] [PDF] |
||||
![]() |
K. Essin, A. Welling, F. Hofmann, F. C. Luft, M. Gollasch, and S. Moosmang Indirect coupling between Cav1.2 channels and ryanodine receptors to generate Ca2+ sparks in murine arterial smooth muscle cells J. Physiol., October 1, 2007; 584(1): 205 - 219. [Abstract] [Full Text] [PDF] |
||||
![]() |
T. Kamishima, T. Burdyga, J. A. Gallagher, and J. M. Quayle Caveolin-1 and caveolin-3 regulate Ca2+ homeostasis of single smooth muscle cells from rat cerebral resistance arteries Am J Physiol Heart Circ Physiol, July 1, 2007; 293(1): H204 - H214. [Abstract] [Full Text] [PDF] |
||||
![]() |
A. Adebiyi, G. Zhao, S. Y. Cheranov, A. Ahmed, and J. H. Jaggar Caveolin-1 abolishment attenuates the myogenic response in murine cerebral arteries Am J Physiol Heart Circ Physiol, March 1, 2007; 292(3): H1584 - H1592. [Abstract] [Full Text] [PDF] |
||||
| ||||||||||||||||||||||||||||||||||||||||||||||||||||||||