TY  - JOUR
A1  - Zaho, Huaying
A1  - Ghirlando, Rodolfo
A1  - Alfonso, Carlos
A1  - Arisaka, Fumio
A1  - Attali, Ilan
A1  - Bain, David L.
A1  - Bakhtina, Marina M.
A1  - Becker, Donald F.
A1  - Bedwell, Gregory J.
A1  - Bekdemir, Ahmet
A1  - Besong, Tabot M. D.
A1  - Birck, Catherine
A1  - Brautigam, Chad A.
A1  - Brennerman, William
A1  - Byron, Olwyn
A1  - Bzowska, Agnieszka
A1  - Chaires, Jonathan B.
A1  - Chaton, Catherine T.
A1  - Coelfen, Helmbut
A1  - Connaghan, Keith D.
A1  - Crowley, Kimberly A.
A1  - Curth, Ute
A1  - Daviter, Tina
A1  - Dean, William L.
A1  - Diez, Ana I.
A1  - Ebel, Christine
A1  - Eckert, Debra M.
A1  - Eisele, Leslie E.
A1  - Eisenstein, Edward
A1  - England, Patrick
A1  - Escalante, Carlos
A1  - Fagan, Jeffrey A.
A1  - Fairman, Robert
A1  - Finn, Ron M.
A1  - Fischle, Wolfgang
A1  - Garcia de la Torre, Jose
A1  - Gor, Jayesh
A1  - Gustafsson, Henning
A1  - Hall, Damien
A1  - Harding, Stephen E.
A1  - Hernandez Cifre, Jose G.
A1  - Herr, Andrew B.
A1  - Howell, Elizabeth E.
A1  - Isaac, Richard S.
A1  - Jao, Shu-Chuan
A1  - Jose, Davis
A1  - Kim, Soon-Jong
A1  - Kokona, Bashkim
A1  - Kornblatt, Jack A.
A1  - Kosek, Dalibor
A1  - Krayukhina, Elena
A1  - Krzizike, Daniel
A1  - Kusznir, Eric A.
A1  - Kwon, Hyewon
A1  - Larson, Adam
A1  - Laue, Thomas M.
A1  - Le Roy, Aline
A1  - Leech, Andrew P.
A1  - Lilie, Hauke
A1  - Luger, Karolin
A1  - Luque-Ortega, Juan R.
A1  - Ma, Jia
A1  - May, Carrie A.
A1  - Maynard, Ernest L.
A1  - Modrak-Wojcik, Anna
A1  - Mok, Yee-Foong
A1  - Mücke, Norbert
A1  - Nagel-Steger, Luitgard
A1  - Narlikar, Geeta J.
A1  - Noda, Masanori
A1  - Nourse, Amanda
A1  - Obsil, Thomas
A1  - Park, Chad K
A1  - Park, Jin-Ku
A1  - Pawelek, Peter D.
A1  - Perdue, Erby E.
A1  - Perkins, Stephen J.
A1  - Perugini, Matthew A.
A1  - Peterson, Craig L.
A1  - Peverelli, Martin G.
A1  - Piszczek, Grzegorz
A1  - Prag, Gali
A1  - Prevelige, Peter E.
A1  - Raynal, Bertrand D. E.
A1  - Rezabkova, Lenka
A1  - Richter, Klaus
A1  - Ringel, Alison E.
A1  - Rosenberg, Rose
A1  - Rowe, Arthur J.
A1  - Rufer, Arne C.
A1  - Scott, David J.
A1  - Seravalli, Javier G.
A1  - Solovyova, Alexandra S.
A1  - Song, Renjie
A1  - Staunton, David
A1  - Stoddard, Caitlin
A1  - Stott, Katherine
A1  - Strauss, Holder M.
A1  - Streicher, Werner W.
A1  - Sumida, John P.
A1  - Swygert, Sarah G.
A1  - Szczepanowski, Roman H.
A1  - Tessmer, Ingrid
A1  - Toth, Ronald T.
A1  - Tripathy, Ashutosh
A1  - Uchiyama, Susumu
A1  - Uebel, Stephan F. W.
A1  - Unzai, Satoru
A1  - Gruber, Anna Vitlin
A1  - von Hippel, Peter H.
A1  - Wandrey, Christine
A1  - Wang, Szu-Huan
A1  - Weitzel, Steven E
A1  - Wielgus-Kutrowska, Beata
A1  - Wolberger, Cynthia
A1  - Wolff, Martin
A1  - Wright, Edward
A1  - Wu, Yu-Sung
A1  - Wubben, Jacinta M.
A1  - Schuck, Peter
T1  - A Multilaboratory Comparison of Calibration Accuracy and the Performance of External References in Analytical Ultracentrifugation
JF  - PLoS ONE
N2  - Analytical ultracentrifugation (AUC) is a first principles based method to determine absolute sedimentation coefficients and buoyant molar masses of macromolecules and their complexes, reporting on their size and shape in free solution. The purpose of this multi-laboratory study was to establish the precision and accuracy of basic data dimensions in AUC and validate previously proposed calibration techniques. Three kits of AUC cell assemblies containing radial and temperature calibration tools and a bovine serum albumin (BSA) reference sample were shared among 67 laboratories, generating 129 comprehensive data sets. These allowed for an assessment of many parameters of instrument performance, including accuracy of the reported scan time after the start of centrifugation, the accuracy of the temperature calibration, and the accuracy of the radial magnification. The range of sedimentation coefficients obtained for BSA monomer in different instruments and using different optical systems was from 3.655 S to 4.949 S, with a mean and standard deviation of (4.304\(\pm\)0.188) S (4.4%). After the combined application of correction factors derived from the external calibration references for elapsed time, scan velocity, temperature, and radial magnification, the range of s-values was reduced 7-fold with a mean of 4.325 S and a 6-fold reduced standard deviation of \(\pm\)0.030 S (0.7%). In addition, the large data set provided an opportunity to determine the instrument-to-instrument variation of the absolute radial positions reported in the scan files, the precision of photometric or refractometric signal magnitudes, and the precision of the calculated apparent molar mass of BSA monomer and the fraction of BSA dimers. These results highlight the necessity and effectiveness of independent calibration of basic AUC data dimensions for reliable quantitative studies.
KW  - fluorescence-detected sedimentation
KW  - size exclusion chromatography
KW  - field flow fractionation
KW  - spinco ultracentrifuge
KW  - aggregation
KW  - bead models
KW  - velocity
KW  - hydrodynamics
KW  - biopharmaceuticals
KW  - proteins
Y1  - 2015
U6  - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-151903
VL  - 10
IS  - 5
ER  - 
TY  - THES
A1  - Richter, Stephan
T1  - Detaillierte Simulationen von Blazar-Emissionen : ein numerischer Zugang zu Radiobeobachtungen und Kurzzeitvariabilität
T1  - Detailed Simulations of Blazar-Emission: A numerical approach to Radio observations and short term variability
N2  - Die vorliegende Arbeit beschäftigt sich mit den Prozessen, die in einer Unterklasse der Aktiven Galaxienkerne, den Blazaren, das Emissionsspektrum dieser Objekte erzeugen. Dies beinhaltet insbesondere den Beschleunigungsprozess, der eine nichtthermische Teilchenverteilung erzeugt, sowie diverse Strahlungsprozesse. Das Spektrum dieser Quellen reicht dabei vom Radiobereich bis zu Energien im TeV-Bereich. Die Form des zeitlich gemittelten Spektrums kann durch Modelle bereits sehr gut beschrieben werden. Insbesondere die erste der beiden dominierenden Komponenten des Spektrums kann mit hoher Sicherheit mit Synchrotronemission einer Elektronenenergieverteilung in Form eines Potenzgesetzes identifiziert werden. Für den Ursprung der zweiten Komponente existieren jedoch verschiedene Erklärungsversuche. Dies sind im wesentlichen die inverse Compton-Streuung der internen oder externer Strahlung (leptonische Modelle) sowie die Emission und photohadronische Wechselwirkung einer hochenergetischen Verteilung von Protonen in der Quelle.

Eine räumliche Auflösung des Ursprungs der detektierten Strahlung ist mit den zur Verfügung stehenden Teleskopen nicht möglich. Einschränkungen für die Ausdehnung dieser Emissionszone ergeben sich lediglich aus der Variation des Emissionsspektrums. Eine Bestimmung der Morphologie ist jedoch im selbstabsorbierten Radiobereich des Spektrums durch die Ausnutzung von interferometrischen Beobachtungen möglich. Die resultierenden Längen, auf denen die im inneren der Quelle selbstabsorbierte Strahlung die Quelle schließlich verlässt, sind jedoch etwa zwei Größenordnungen oberhalb der aus den Variabilitätszeitskalen gefolgerten Limits.

Das im Rahmen dieser Arbeit entwickelte Modell soll dabei helfen, verschiedene Beobachtungen mit Hilfe eines quantitativen Modells zu beschreiben. Hier steht insbesondere die Korrelation zwischen den Verläufen der Hochenergie- und Radioemission im Vordergrund. Eine Aussage über die Existenz einer solchen Verbindung konnte aus den bisherigen Beobachtungen nicht getroffen werden.
Eine quantitative Modellierung könnte bei der Interpretation der bisher uneindeutigen Datenlage helfen. Eine weitere, durch Modelle bisher nicht beschreibbare, Beobachtungsevidenz sind extrem kurzzeitige Variationen des Flusszustands.
Die Lichtlaufzeit durch das für die Modellierung benötigte Raumgebiet ist zumeist größer als die beobachtete Zeitskala.
Zudem deuten die Beobachtungen darauf hin, dass manche dieser Flussausbrüche nicht zwischen den verschiedenen Bändern korreliert sind, wie es zumindest die leptonischen Modelle erwarten lassen würden.

Das hier beschriebene Modell verbindet eine räumliche Auflösung des Emissionsgebiets mit dem dominanten Beschleunigungsmechanismus. Hierdurch konnte zunächst gezeigt werden, dass die Beschreibung von Variabilität auch auf Skalen unterhalb der Lichtlaufzeit durch das modellierte Raumgebiet möglich ist. Zudem wurde ein Szenario quantifiziert, dass im leptonischen Fall unkorrelierte Ausbrüche vorhersagt.
\thispagestyle{empty}
Durch eine Erweiterung des Emissionsgebiets gegenüber anderen Blazar-Modellen um zwei Größenordnung konnte zudem eine Verknüpfung zwischen dem Hochenergie- und dem Radiobereich erfolgen. Die gefundene Morphologie des Einschlussgebiets der nichtthermischen Teilchenpopulation beinhaltet eine physikalisch sinnvolle Randbedingung für das Emissionsgebiet der Hochenergiestrahlung, die zudem den für die betrachtete Quelle korrekten Spektralindex im Radiobereich erzeugt.
Darüber hinaus wurden in das Modell sowohl leptonische als auch hadronische Prozesse integriert, die eine flexible und unvoreingenommene Modellierung potentieller Hybridquellen erlauben.

Mit dem entwickelten Modell ist es möglich, aus detailliert vermessenen Lichtkurven im Hochenergiebereich die zu erwartende Radioemission vorherzusagen. Die in diese Vorhersage eingehenden Parameter lassen sich aus der Modellierung des Gleichgewichtsspektrums bestimmen.
N2  - The work presented here addresses processes that are responsible for the emission spectra of a certain sub-class of Active Galactic Nuclei, the Blazars. In particular, these include the acceleration process,
producing the non-thermal particle distribution, and various Emission processes. The spectra of Blazars range from the radio band up until energies in the TeV range. The form of the steady state spectrum is explained well by existing models. There is, in particular, strong
evidence that the first of the two bumps of the spectral energy distribution is the synchrotron emission of an electron power-law distribution. For the second bump there are, however, several possibilities. Roughly speaking these are the inverse Compton scattering of
the internal radiation or an external radiation field (leptonic models), as well as the emission of non-thermal protons and photo hadronic interactions with these protons.

A resolution of the source of the detected radiation is not in the scope of existing telescopes. Limits on the spatial extent of the Emission region only follow from the variation timescales of the spectra. In the
self-absorbed radio regime, a determination of the morphology is however possible due to interferometric observations. The observed lengths represent the scale at which the radiation, which is self-absorbed in
the innermost parts, eventually leaves the source. However, this scale is two orders of magnitude larger than the limits deduced from the variability timescales.

The model developed during the course of this work is designed to produce a quantitative description of various observations. First and foremost these are the correlations between the radio regime and the very high energy regime. Strong evidence either for or against the existence of such a correlation was not possible thus far with the available data. Quantitative modelling could help to interpret the presently unclear situation. Additional observations, that cannot be explained by current models, are extreme short-term variability. The light travelling times through the emission region that are required for the steady state modelling are usually much longer than the observed timescales. Moreover,
observations indicate that some of the observed flares have no correlated variability in other bands as would be expected from leptonic models.

The model described in this thesis connects a spatial resolution of the emission region with the dominant acceleration process. With this approach it could be shown, that the modelling of variability on scales
below the light travel time limits can be achieved. Moreover, a leptonic scenario predicting uncorrelated short-term variability was quantified.
A connection between the radio and very high energy emission was achieved via an extension of the size of the emission region by two orders of magnitude. The morphology of the confinement region that was
used for the large scale simulations provides both a physical Sound boundary condition for the high energy emission, as well as a correct description of the observed spectral index in the radio.
Furthermore, both leptonic and photohadronic processes were implemented, providing a flexible and unbiased modelling of hybrid sources.

The developed model is capable of predicting the radio emission on the basis of detailed light curves in the high energy regime. The Parameters entering this prediction follow from the modelling of the steady state
of the chosen source.
KW  - Blazar
KW  - Strahlung
KW  - Mathematisches Modell
KW  - Strahlung
Y1  - 2014
U6  - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-103209
ER  - 
TY  - JOUR
A1  - Davis, Lea K.
A1  - Yu, Dongmei
A1  - Keenan, Clare L.
A1  - Gamazon, Eric R.
A1  - Konkashbaev, Anuar I.
A1  - Derks, Eske M.
A1  - Neale, Benjamin M.
A1  - Yang, Jian
A1  - Lee, S. Hong
A1  - Evans, Patrick
A1  - Barr, Cathy L.
A1  - Bellodi, Laura
A1  - Benarroch, Fortu
A1  - Berrio, Gabriel Bedoya
A1  - Bienvenu, Oscar J.
A1  - Bloch, Michael H.
A1  - Blom, Rianne M.
A1  - Bruun, Ruth D.
A1  - Budman, Cathy L.
A1  - Camarena, Beatriz
A1  - Campbell, Desmond
A1  - Cappi, Carolina
A1  - Cardona Silgado, Julio C.
A1  - Cath, Danielle C.
A1  - Cavallini, Maria C.
A1  - Chavira, Denise A.
A1  - Chouinard, Sylvian
A1  - Conti, David V.
A1  - Cook, Edwin H.
A1  - Coric, Vladimir
A1  - Cullen, Bernadette A.
A1  - Deforce, Dieter
A1  - Delorme, Richard
A1  - Dion, Yves
A1  - Edlund, Christopher K.
A1  - Egberts, Karin
A1  - Falkai, Peter
A1  - Fernandez, Thomas V.
A1  - Gallagher, Patience J.
A1  - Garrido, Helena
A1  - Geller, Daniel
A1  - Girard, Simon L.
A1  - Grabe, Hans J.
A1  - Grados, Marco A.
A1  - Greenberg, Benjamin D.
A1  - Gross-Tsur, Varda
A1  - Haddad, Stephen
A1  - Heiman, Gary A.
A1  - Hemmings, Sian M. J.
A1  - Hounie, Ana G.
A1  - Illmann, Cornelia
A1  - Jankovic, Joseph
A1  - Jenike, Micheal A.
A1  - Kennedy, James L.
A1  - King, Robert A.
A1  - Kremeyer, Barbara
A1  - Kurlan, Roger
A1  - Lanzagorta, Nuria
A1  - Leboyer, Marion
A1  - Leckman, James F.
A1  - Lennertz, Leonhard
A1  - Liu, Chunyu
A1  - Lochner, Christine
A1  - Lowe, Thomas L.
A1  - Macciardi, Fabio
A1  - McCracken, James T.
A1  - McGrath, Lauren M.
A1  - Restrepo, Sandra C. Mesa
A1  - Moessner, Rainald
A1  - Morgan, Jubel
A1  - Muller, Heike
A1  - Murphy, Dennis L.
A1  - Naarden, Allan L.
A1  - Ochoa, William Cornejo
A1  - Ophoff, Roel A.
A1  - Osiecki, Lisa
A1  - Pakstis, Andrew J.
A1  - Pato, Michele T.
A1  - Pato, Carlos N.
A1  - Piacentini, John
A1  - Pittenger, Christopher
A1  - Pollak, Yehunda
A1  - Rauch, Scott L.
A1  - Renner, Tobias J.
A1  - Reus, Victor I.
A1  - Richter, Margaret A.
A1  - Riddle, Mark A.
A1  - Robertson, Mary M.
A1  - Romero, Roxana
A1  - Rosàrio, Maria C.
A1  - Rosenberg, David
A1  - Rouleau, Guy A.
A1  - Ruhrmann, Stephan
A1  - Ruiz-Linares, Andreas
A1  - Sampaio, Aline S.
A1  - Samuels, Jack
A1  - Sandor, Paul
A1  - Sheppard, Broke
A1  - Singer, Harvey S.
A1  - Smit, Jan H.
A1  - Stein, Dan J.
A1  - Strengman, E.
A1  - Tischfield, Jay A.
A1  - Valencia Duarte, Ana V.
A1  - Vallada, Homero
A1  - Van Nieuwerburgh, Flip
A1  - Veenstra-VanderWeele, Jeremy
A1  - Walitza, Susanne
A1  - Wang, Ying
A1  - Wendland, Jens R.
A1  - Westenberg, Herman G. M.
A1  - Shugart, Yin Yao
A1  - Miguel, Euripedes C.
A1  - McMahon, William
A1  - Wagner, Michael
A1  - Nicolini, Humberto
A1  - Posthuma, Danielle
A1  - Hanna, Gregory L.
A1  - Heutink, Peter
A1  - Denys, Damiaan
A1  - Arnold, Paul D.
A1  - Oostra, Ben A.
A1  - Nestadt, Gerald
A1  - Freimer, Nelson B.
A1  - Pauls, David L.
A1  - Wray, Naomi R.
A1  - Stewart, S. Evelyn
A1  - Mathews, Carol A.
A1  - Knowles, James A.
A1  - Cox, Nancy J.
A1  - Scharf, Jeremiah M.
T1  - Partitioning the Heritability of Tourette Syndrome and Obsessive Compulsive Disorder Reveals Differences in Genetic Architecture
JF  - PLoS Genetics
N2  - The direct estimation of heritability from genome-wide common variant data as implemented in the program Genome-wide Complex Trait Analysis (GCTA) has provided a means to quantify heritability attributable to all interrogated variants. We have quantified the variance in liability to disease explained by all SNPs for two phenotypically-related neurobehavioral disorders, obsessive-compulsive disorder (OCD) and Tourette Syndrome (TS), using GCTA. Our analysis yielded a heritability point estimate of 0.58 (se = 0.09, p = 5.64e-12) for TS, and 0.37 (se = 0.07, p = 1.5e-07) for OCD. In addition, we conducted multiple genomic partitioning analyses to identify genomic elements that concentrate this heritability. We examined genomic architectures of TS and OCD by chromosome, MAF bin, and functional annotations. In addition, we assessed heritability for early onset and adult onset OCD. Among other notable results, we found that SNPs with a minor allele frequency of less than 5% accounted for 21% of the TS heritability and 0% of the OCD heritability. Additionally, we identified a significant contribution to TS and OCD heritability by variants significantly associated with gene expression in two regions of the brain (parietal cortex and cerebellum) for which we had available expression quantitative trait loci (eQTLs). Finally we analyzed the genetic correlation between TS and OCD, revealing a genetic correlation of 0.41 (se = 0.15, p = 0.002). These results are very close to previous heritability estimates for TS and OCD based on twin and family studies, suggesting that very little, if any, heritability is truly missing (i.e., unassayed) from TS and OCD GWAS studies of common variation. The results also indicate that there is some genetic overlap between these two phenotypically-related neuropsychiatric disorders, but suggest that the two disorders have distinct genetic architectures.
KW  - TIC disorders
KW  - missing heritability
KW  - complex diseases
KW  - neuropsychiatric disorders
KW  - common SNPS
KW  - gilles
KW  - family
KW  - brain
KW  - expression
KW  - autism
Y1  - 2013
U6  - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-127377
SN  - 1553-7390
VL  - 9
IS  - 10
ER  - 
TY  - JOUR
A1  - Pittig, Andre
A1  - Heinig, Ingmar
A1  - Goerigk, Stephan
A1  - Thiel, Freya
A1  - Hummel, Katrin
A1  - Scholl, Lucie
A1  - Deckert, Jürgen
A1  - Pauli, Paul
A1  - Domschke, Katharina
A1  - Lueken, Ulrike
A1  - Fydrich, Thomas
A1  - Fehm, Lydia
A1  - Plag, Jens
A1  - Ströhle, Andreas
A1  - Kircher, Tilo
A1  - Straube, Benjamin
A1  - Rief, Winfried
A1  - Koelkebeck, Katja
A1  - Arolt, Volker
A1  - Dannlowski, Udo
A1  - Margraf, Jürgen
A1  - Totzeck, Christina
A1  - Schneider, Silvia
A1  - Neudeck, Peter
A1  - Craske, Michelle G.
A1  - Hollandt, Maike
A1  - Richter, Jan
A1  - Hamm, Alfons
A1  - Wittchen, Hans-Ulrich
T1  - Efficacy of temporally intensified exposure for anxiety disorders: A multicenter randomized clinical trial
JF  - Depression and Anxiety
N2  - Background

The need to optimize exposure treatments for anxiety disorders may be addressed by temporally intensified exposure sessions. Effects on symptom reduction and public health benefits should be examined across different anxiety disorders with comorbid conditions.

Methods

This multicenter randomized controlled trial compared two variants of prediction error-based exposure therapy (PeEx) in various anxiety disorders (both 12 sessions + 2 booster sessions, 100 min/session): temporally intensified exposure (PeEx-I) with exposure sessions condensed to 2 weeks (n = 358) and standard nonintensified exposure (PeEx-S) with weekly exposure sessions (n = 368). Primary outcomes were anxiety symptoms (pre, post, and 6-months follow-up). Secondary outcomes were global severity (across sessions), quality of life, disability days, and comorbid depression.

Results

Both treatments resulted in substantial improvements at post (PeEx-I: d\(_{within}\) = 1.50, PeEx-S: d\(_{within}\) = 1.78) and follow-up (PeEx-I: d\(_{within}\) = 2.34; PeEx-S: d\(_{within}\) = 2.03). Both groups showed formally equivalent symptom reduction at post and follow-up. However, time until response during treatment was 32% shorter in PeEx-I (median = 68 days) than PeEx-S (108 days; TR\(_{PeEx-I}\)-I = 0.68). Interestingly, drop-out rates were lower during intensified exposure. PeEx-I was also superior in reducing disability days and improving quality of life at follow-up without increasing relapse.

Conclusions

Both treatment variants focusing on the transdiagnostic exposure-based violation of threat beliefs were effective in reducing symptom severity and disability in severe anxiety disorders. Temporally intensified exposure resulted in faster treatment response with substantial public health benefits and lower drop-out during the exposure phase, without higher relapse. Clinicians can expect better or at least comparable outcomes when delivering exposure in a temporally intensified manner.
KW  - randomized controlled trial
KW  - anxiety disorders
KW  - exposure therapy
KW  - intensified treatment
KW  - public health
Y1  - 2021
U6  - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-257331
VL  - 38
IS  - 11
ER  - 
TY  - JOUR
A1  - Wagner, Michael
A1  - Sadek, Mirna S.
A1  - Dybkova, Nataliya
A1  - Mason, Fleur E.
A1  - Klehr, Johann
A1  - Firneburg, Rebecca
A1  - Cachorro, Eleder
A1  - Richter, Kurt
A1  - Klapproth, Erik
A1  - Kuenzel, Stephan R.
A1  - Lorenz, Kristina
A1  - Heijman, Jordi
A1  - Dobrev, Dobromir
A1  - El-Armouche, Ali
A1  - Sossalla, Samuel
A1  - Kämmerer, Susanne
T1  - Cellular mechanisms of the anti-arrhythmic effect of cardiac PDE2 overexpression
JF  - International Journal of Molecular Sciences
N2  - Background: Phosphodiesterases (PDE) critically regulate myocardial cAMP and cGMP levels. PDE2 is stimulated by cGMP to hydrolyze cAMP, mediating a negative crosstalk between both pathways. PDE2 upregulation in heart failure contributes to desensitization to β-adrenergic overstimulation. After isoprenaline (ISO) injections, PDE2 overexpressing mice (PDE2 OE) were protected against ventricular arrhythmia. Here, we investigate the mechanisms underlying the effects of PDE2 OE on susceptibility to arrhythmias. Methods: Cellular arrhythmia, ion currents, and Ca\(^{2+}\)-sparks were assessed in ventricular cardiomyocytes from PDE2 OE and WT littermates. Results: Under basal conditions, action potential (AP) morphology were similar in PDE2 OE and WT. ISO stimulation significantly increased the incidence of afterdepolarizations and spontaneous APs in WT, which was markedly reduced in PDE2 OE. The ISO-induced increase in I\(_{CaL}\) seen in WT was prevented in PDE2 OE. Moreover, the ISO-induced, Epac- and CaMKII-dependent increase in I\(_{NaL}\) and Ca\(^{2+}\)-spark frequency was blunted in PDE2 OE, while the effect of direct Epac activation was similar in both groups. Finally, PDE2 inhibition facilitated arrhythmic events in ex vivo perfused WT hearts after reperfusion injury. Conclusion: Higher PDE2 abundance protects against ISO-induced cardiac arrhythmia by preventing the Epac- and CaMKII-mediated increases of cellular triggers. Thus, activating myocardial PDE2 may represent a novel intracellular anti-arrhythmic therapeutic strategy in HF.
KW  - PDE2
KW  - arrhythmia
KW  - CaMKII
KW  - heart failure
Y1  - 2021
U6  - http://nbn-resolving.de/urn/resolver.pl?urn:nbn:de:bvb:20-opus-285888
SN  - 1422-0067
VL  - 22
IS  - 9
ER  -