ROLE OF CAVEOLIN-3 IN THE MODULATION OF HERG POTASSIUM CHANNEL

The human ether-a-go-go-related gene (hERG) encodes the pore-forming subunit of the rapidly activating delayed rectifier potassium channel (IKr) that is important for cardiac repolarization. Previously, we have discovered that hERG channels rapidly internalize in low extracellular K+ ([K+]o). In cell culture, this process is driven by the endocytic protein, caveolin-1 (Cav1), which is an integral player in the caveolae-dependant endocytosis pathway. However, in the heart, Caveolin-3 (Cav3) is, in fact, the predominant form in the myocyte, and thus may play a direct role in regulating hERG expression in the heart. Thus, I hypothesize that this reduction of hERG conductance in cardiac myocytes derives from the presence of Cav3, which is integral regulator of hERG homeostasis innately in the heart. To investigate the effect of Cav3 on hERG, I overexpressed Cav3 in human embryonic kidney 293 (HEK-293) cells stably expressing hERG channels. Cav3 overexpression significantly and specifically decreased both the hERG current amplitude and the mature channel expression in normal culture conditions. Co-immunoprecipitation analysis and confocal imaging demonstrated an association between hERG and Cav3 in HEK cells as well as rat and rabbit cardiomyocytes. Mechanistically, I discovered that Cav3 possesses a faster turnover rate compared to Cav1, and can enhance hERG degradation through up-regulating mature channel ubiquitination via the ubiquitin ligase, NEDD4-2. Knockdown of Cav3 in neonatal cardiac myocytes also enhanced hERG expression. My data indicate that Cav3 participates in hERG trafficking, and is an important regulator of hERG channel homeostasis in cardiac myocytes. This information provides a platform for future intervention of the hERG-induced type-2 long QT syndrome (LQTS).

Proton Formation in 2+1 Resonance Enhanced Multiphoton Excitation of HCl and HBr via „=0… Rydberg and Ion-Pair States

Molecular beam cooled HCl was state selected by two-photon excitation of the V (1) summation operator(0(+)) [v=9,11-13,15], E (1) summation operator(0(+)) [v=0], and g (3) summation operator(-)(0(+)) [v=0] states through either the Q(0) or Q(1) lines of the respective (1,3) summation operator(0(+))<--<--X (1) summation operator(0(+)) transition. Similarly, HBr was excited to the V (1) summation operator(0(+)) [v=m+3, m+5-m+8], E (1) summation operator(0(+)) [v=0], and H (1) summation operator(0(+)) [v=0] states through the Q(0) or Q(1) lines. Following absorption of a third photon, protons were formed by three different mechanisms and detected using velocity map imaging. (1) H(*)(n=2) was formed in coincidence with (2)P(i) halogen atoms and subsequently ionized. For HCl, photodissociation into H(*)(n=2)+Cl((2)P(12)) was dominant over the formation of Cl((2)P(32)) and was attributed to parallel excitation of the repulsive [(2) (2)Pi4llambda] superexcited (Omega=0) states. For HBr, the Br((2)P(32))Br((2)P(12)) ratio decreases with increasing excitation energy. This indicates that both the [(3) (2)Pi(12)5llambda] and the [B (2) summation operator5llambda] superexcited (Omega=0) states contribute to the formation of H(*)(n=2). (2) For selected intermediate states HCl was found to dissociate into the H(+)+Cl(-) ion pair with over 20% relative yield. A mechanism is proposed by which a bound [A (2) summation operatornlsigma] (1) summation operator(0(+)) superexcited state acts as a gateway state to dissociation into the ion pair. (3) For all intermediate states, protons were formed by dissociation of HX(+)[v(+)] following a parallel, DeltaOmega=0, excitation. The quantum yield for the dissociation process was obtained using previously reported photoionization efficiency data and was found to peak at v(+)=6-7 for HCl and v(+)=12 for HBr. This is consistent with excitation of the repulsive A(2) summation operator(12) and (2) (2)Pi states of HCl(+), and the (3) (2)Pi state of HBr(+). Rotational alignment of the Omega=0(+) intermediate states is evident from the angular distribution of the excited H(*)(n=2) photofragments. This effect has been observed previously and was used here to verify the reliability of the measured spatial anisotropy parameters.