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Cytosolic re-localization and optimization of valine synthesis and catabolism enables increased isobutanol production with the yeast Saccharomyces cerevisiae

Dawid Brat; Christian Weber; Wolfram Lorenzen; Helge Björn Bode; Eckhard Boles — Mon, 08 Oct 2012 16:47:57 +0200

Background: The branched chain alcohol isobutanol exhibits superior physicochemical properties as an alternative biofuel. The yeast Saccharomyces cerevisiae naturally produces low amounts of isobutanol as a by-product during fermentations, resulting from the catabolism of valine. As S. cerevisiae is widely used in industrial applications and can easily be modified by genetic engineering, this microorganism is a promising host for the fermentative production of higher amounts of isobutanol. Results: Isobutanol production could be improved by re-locating the valine biosynthesis enzymes Ilv2, Ilv5 and Ilv3 from the mitochondrial matrix into the cytosol. To prevent the import of the three enzymes into yeast mitochondria, N-terminally shortened Ilv2, Ilv5 and Ilv3 versions were constructed lacking their mitochondrial targeting sequences. SDS-PAGE and immunofluorescence analyses confirmed expression and re-localization of the truncated enzymes. Growth tests or enzyme assays confirmed enzymatic activities. Isobutanol production was only increased in the absence of valine and the simultaneous blockage of the mitochondrial valine synthesis pathway. Isobutanol production could be even more enhanced after adapting the codon usage of the truncated valine biosynthesis genes to the codon usage of highly expressed glycolytic genes. Finally, a suitable ketoisovalerate decarboxylase, Aro10, and alcohol dehydrogenase, Adh2, were selected and overexpressed. The highest isobutanol titer was 0.63 g/L at a yield of nearly 15 mg per g glucose. Conclusion: A cytosolic isobutanol production pathway was successfully established in yeast by re-localization and optimization of mitochondrial valine synthesis enzymes together with overexpression of Aro10 decarboxylase and Adh2 alcohol dehydrogenase. Driving forces were generated by blocking competition with the mitochondrial valine pathway and by omitting valine from the fermentation medium. Additional deletion of pyruvate decarboxylase genes and engineering of co-factor imbalances should lead to even higher isobutanol production.

Gender differences in associations of glutamate decarboxylase 1 gene (GAD1) variants with panic disorder

Fri, 01 Jun 2012 09:50:21 +0200

Background: Panic disorder is common (5% prevalence) and females are twice as likely to be affected as males. The heritable component of panic disorder is estimated at 48%. Glutamic acid dehydrogenase GAD1, the key enzyme for the synthesis of the inhibitory and anxiolytic neurotransmitter GABA, is supposed to influence various mental disorders, including mood and anxiety disorders. In a recent association study in depression, which is highly comorbid with panic disorder, GAD1 risk allele associations were restricted to females. Methodology/Principal Findings: Nineteen single nucleotide polymorphisms (SNPs) tagging the common variation in GAD1 were genotyped in two independent gender and age matched case-control samples (discovery sample n = 478; replication sample n = 584). Thirteen SNPs passed quality control and were examined for gender-specific enrichment of risk alleles associated with panic disorder by using logistic regression including a genotype×gender interaction term. The latter was found to be nominally significant for four SNPs (rs1978340, rs3762555, rs3749034, rs2241165) in the discovery sample; of note, the respective minor/risk alleles were associated with panic disorder only in females. These findings were not confirmed in the replication sample; however, the genotype×gender interaction of rs3749034 remained significant in the combined sample. Furthermore, this polymorphism showed a nominally significant association with the Agoraphobic Cognitions Questionnaire sum score. Conclusions/Significance: The present study represents the first systematic evaluation of gender-specific enrichment of risk alleles of the common SNP variation in the panic disorder candidate gene GAD1. Our tentative results provide a possible explanation for the higher susceptibility of females to panic disorder.

Identifizierung und Charakterisierung der mRNA processing bodies von Arabidopsis thaliana

Christian Weber — Wed, 03 Sep 2008 10:47:03 +0200

mRNA-Abbau ist ein essentieller Prozess der Genexpression, der den Zellen ermöglicht, die Qualität und die Quantität der mRNA zu kontrollieren. Besonders unter Stressbedingungen könnte der mRNA-Abbau eine bedeutende Rolle neben der Speicherung von mRNAs sowie der Regulation der Proteinhomöostase zum Schutz vor schädigenden Einflüssen spielen. Studien mit Hefen und Säugerzellen zeigten, dass dem 5'-3'mRNA-Abbau ein wichtige Rolle sowohl unter normalen Bedingungen als auch unter Stressbedingungen zukommt und dieser in zytoplasmatischen Processing bodies (P-bodies) stattfindet. Im Rahmen dieser Arbeit sollten Erkenntnisse über den 5'-3'mRNA-Abbau erhalten werden. Im Vordergrund stand die Frage nach der Existenz von P-bodies in Arabidopsis thaliana und die Identifikation und Charakterisierung deren Komponenten. Weiterhin sollten Erkenntnisse über die Rolle der P-bodies unter Stressbedingungen gewonnen werden. Dabei sollten besonders Informationen über die Beziehungen zwischen den P-bodies und RNA Stressgranula (mRNA Speicherkompartimente) und Hitzestressgranula (Regulation der Proteinhomöostase) erhalten werden. Das komplette sequenzierte Genom von Arabidopsis thaliana eignete sich zur Identifikation von mRNA-Abbauproteine kodierender Gene. Unter Verwendung von Aminosäuresequenzen bereits bekannter mRNA-Abbauproteine aus Hefe und Säugerzellen konnten Homologe für die Decappingproteine Dcp1 und Dcp2 sowie für die Proteine LSm1,2,5,8 als Untereinheiten des LSm1-7 Komplexes, welcher an der Regulation der Decappingreaktion beteiligt ist, identifiziert werden. Über Hefe-Zwei-Hybrid Analysen konnten anschließend Protein-Protein-Interaktionen zwischen den untersuchten Proteinen identifiziert werden. Weiterhin konnte unter Einsatz der BIFC-Analyse gezeigt werden, dass die Interaktionen zwischen den untersuchten Proteinen hauptsächlich in zytoplasmatischen Strukturen stattfanden. Aufbauend auf diesen Befunden wurde ein Antikörper gegen Dcp1 als Marker für die zytoplasmatischen Strukturen erstellt. Dieser ermöglichte erstmals die Detektion der endogenen Strukturen in Arabidopsis thaliana. Die weitere Charakterisierung über Immunofluoreszenzanalysen zeigten, dass diese P-bodies sind. Wie die P-bodies anderer Organismen sind sie hochdynamisch und benötigen untranslatierte mRNA für die Assemblierung. Die Größe und Anzahl der P-bodies hängt dabei vom Verhältniss des Zuflusses von mRNA und der mRNA-Abbaurate ab. Weiterhin konnte beobachtet werden, das die P-bodies besonders groß unter Stressbedingungen sind und deuten eine wichtige Funktion des mRNA-Abbaus unter Stress an. Dies führte zu der Frage nach der Beziehung der P-bodies zu RNA Stressgranula, die der Speicherung von mRNA unter Stressbedingungen dienen, sowie zu Hitzestressgranula, die an der Aufrechterhaltung der Proteinhomöostase beteiligt sind. Durch Kolokalisationsanalysen mit Markern der RNA Stressgranula, der Hitzestressgranula und der P-bodies konnte erstmals gezeigt werden, dass es sich um voneinander unabhängige Mikrokompartimente handelt, und dass unter Stressbedingungen die zellulären Prozesse mRNA-Abbau, mRNA-Speicherung und Aufrechterhaltung der Proteinhomöostase auf einzelne Mikrkompartimente beschränkt sind. Allerdings konnte zwischen P-bodies und RNA Stressgranula häufig eine räumliche Nähe beobachtet werden. Dies deutet auf einen Austausch von Komponenten zwischen diesen Strukturen hin. Zusammen zeigen die erhaltenen Ergebnisse, dass die identifizierten Proteine Komponenten des 5'-3'mRNA-Abbaus darstellen, und dass der 5'-3'mRNA-Abbau in Pflanzen auch in P-bodies stattfindet. Die Identifizierung und Charakterisierung der pflanzlichen P-bodies bildet eine Grundlage für zukünftige Untersuchungen. Vor allem die massive Bildung von P-bodies unter Stressbedingungen und die Interaktion der P-bodies mit RNA Stressgranula zeigen neue Aspekte der pflanzlichen Hitzestressantwort auf.

Nucleus-nucleus collisions at highest energies

Mon, 23 Jan 2006 10:08:06 +0100

The microscopic phasespace approach URQMD is used to investigate the stopping power and particle production in heavy systems at SPS and RHIC energies. We find no gap in the baryon rapidity distribution even at RHIC. For CERN energies URQMD shows a pile up of baryons and a supression of multi-nucleon clusters at midrapidity.

Fluctuations and inhomogenities of energy density and isospin in Pb + Pb at the SPS

Thu, 15 Dec 2005 13:51:45 +0100

The main goal of heavy ion physics in the last fifteen years has been the search for the quark-gluon-plasma(QGP). Until now, unambigous experimental evidence for the QGP is missing.

Can momentum correlations proof kinetic equilibration in heavy ion collisions at 160/A-GeV?

Wed, 14 Dec 2005 13:32:36 +0100

We perform an event-by-event analysis of the transverse momentum distribution of final state particles in central Pb(160AGeV)+Pb collisions within a microscopic non-equilibrium transport model (UrQMD). Strong influence of rescattering is found. The extracted momentum distributions show less fluctuations in A+A collisions than in p+p reactions. This is in contrast to simplified p+p extrapolations and random walk models.

Excitation function of energy density and partonic degrees of freedom in relativistic heavy ion collisions

Fri, 09 Dec 2005 10:24:09 +0100

We estimate the energy density epsilon pile-up at mid-rapidity in central Pb+Pb collisions from 2 200 GeV/nucleon. epsilon is decomposed into hadronic and partonic contributions. A detailed analysis of the collision dynamics in the framework of a microscopic transport model shows the importance of partonic degrees of freedom and rescattering of leading (di)quarks in the early phase of the reaction for Elab 30 GeV/nucleon. In Pb+Pb collisions at 160 GeV/nucleon the energy density reaches up to 4 GeV/fm3, 95% of which are contained in partonic degrees of freedom.

Equilibrium and nonequilibrium effects in nucleus nucleus collisions

Wed, 07 Dec 2005 13:22:18 +0100

Abstract: Local thermal and chemical equilibration is studied for central AqA collisions at 10.7 160 AGeV in the Ultrarelativis- . tic Quantum Molecular Dynamics model UrQMD . The UrQMD model exhibits strong deviations from local equilibrium at the high density hadron string phase formed during the early stage of the collision. Equilibration of the hadron resonance matter is established in the central cell of volume Vs125 fm3 at later stages, tG10 fmrc, of the resulting quasi-isentropic expansion. The thermodynamical functions in the cell and their time evolution are presented. Deviations of the UrQMD quasi-equilibrium state from the statistical mechanics equilibrium are found. They increase with energy per baryon and lead to a strong enhancement of the pion number density as compared to statistical mechanics estimates at SPS energies. PACS: 25.75.-q; 24.10.Lx; 24.10.Pa; 64.30.qt

Critical review of quark gluon plasma signatures

Wed, 07 Dec 2005 10:33:38 +0100

Noneequilibrium models (three-fluid hydrodynamics and UrQMD) use to discuss the uniqueness of often proposed experimental signatures for quark matter formation in relativistic heavy ion collisions. It is demonstrated that these two models - although they do treat the most interesting early phase of the collisions quite differently(thermalizing QGP vs. coherent color fields with virtual particles) - both yields a reasonable agreement with a large variety of the available heavy ion data.

Relativistic hadron-hadron collisions in the ultra-relativistic quantum molecular dynamics model

Thu, 24 Nov 2005 10:50:57 +0100

Hadron-hadron collisions at high energies are investigated in the Ultra- relativistic-Quantum-Molecular-Dynamics approach. This microscopic trans- port model describes the phenomenology of hadronic interactions at low and intermediate energies ( s < 5 GeV) in terms of interactions between known hadrons and their resonances. At higher energies, s > 5 GeV, the excitation of color strings and their subsequent fragmentation into hadrons dominates the multiple production of particles in the UrQMD model. The model shows a fair overall agreement with a large body of experimental h-h data over a wide range of h-h center-of-mass energies. Hadronic reaction data with higher precision would be useful to support the use of the UrQMD model for relativistic heavy ion collisions.

Physics opportunities at RHIC and LHC

Tue, 01 Nov 2005 09:26:33 +0100

Nonequilibrium models (three-fluid hydrodynamics, UrQMD, and quark molecular dynamics) are used to discuss the uniqueness of often proposed experimental signatures for quark matter formation in relativistic heavy ion collisions from the SPS via RHIC to LHC. It is demonstrated that these models - although they do treat the most interesting early phase of the collisions quite differently (thermalizing QGP vs. coherent color fields with virtual particles) -- all yield a reasonable agreement with a large variety of the available heavy ion data. Hadron/hyperon yields, including J/Psi meson production/suppression, strange matter formation, dileptons, and directed flow (bounce-off and squeeze-out) are investigated. Observations of interesting phenomena in dense matter are reported. However, we emphasize the need for systematic future measurements to search for simultaneous irregularities in the excitation functions of several observables in order to come close to pinning the properties of hot, dense QCD matter from data. The role of future experiments with the STAR and ALICE detectors is pointed out.

Current status of quark gluon plasma signals

Thu, 14 Apr 2005 16:28:30 +0200

Compelling evidence for the creation of a new form of matter has been claimed to be found in Pb+Pb collisions at SPS. We discuss the uniqueness of often proposed experimental signatures for quark matter formation in relativistic heavy ion collisions. It is demonstrated that so far none of the proposed signals like J/psi meson production/suppression, strangeness enhancement, dileptons, and directed flow unambigiously show that a phase of deconfined matter has been formed in SPS Pb+Pb collisions. We emphasize the need for systematic future measurements to search for simultaneous irregularities in the excitation functions of several observables in order to come close to pinning the properties of hot, dense QCD matter from data.

Chemical freeze-out parameters at RHIC from microscopic model calculations

Thu, 14 Apr 2005 15:54:10 +0200

The relaxation of hot nuclear matter to an equilibrated state in the central zone of heavy-ion collisions at energies from AGS to RHIC is studied within the microscopic UrQMD model. It is found that the system reaches the (quasi)equilibrium stage for the period of 10-15 fm/c. Within this time the matter in the cell expands nearly isentropically with the entropy to baryon ratio S/A = 150 - 170. Thermodynamic characteristics of the system at AGS and at SPS energies at the endpoints of this stage are very close to the parameters of chemical and thermal freeze-out extracted from the thermal fit to experimental data. Predictions are made for the full RHIC energy square root s = 200$ AGeV. The formation of a resonance-rich state at RHIC energies is discussed.

Microscopic calculations of stopping and flow from 160AMeV to 160AGeV

Thu, 14 Apr 2005 15:45:00 +0200

The behavior of hadronic matter at high baryon densities is studied within Ultrarelativistic Quantum Molecular Dynamics (URQMD). Baryonic stopping is observed for Au+Au collisions from SIS up to SPS energies. The excitation function of flow shows strong sensitivities to the underlying equation of state (EOS), allowing for systematic studies of the EOS. Effects of a density dependent pole of the rho-meson propagator on dilepton spectra are studied for different systems and centralities at CERN energies.

Signatures of dense hadronic matter in ultrarelativistic heavy ion reactions

Thu, 14 Apr 2005 14:41:59 +0200

The behavior of hadronic matter at high baryon densities is studied within Ultrarelativistic Quantum Molecular Dynamics (URQMD). Baryonic stopping is observed for Au+Au collisions from SIS up to SPS energies. The excitation function of flow shows strong sensitivities to the underlying equation of state (EOS), allowing for systematic studies of the EOS. Dilepton spectra are calculated with and without shifting the rho pole. Except for S+Au collisions our calculations reproduce the CERES data.

Collective flow in heavy ion reactions and the properties of excited nuclear matter

Thu, 14 Apr 2005 14:29:03 +0200

Quantum Molecular Dynamics (QMD) calculations of central collisions between heavy nuclei are used to study fragment production and the creation of collective flow. It is shown that the final phase space distributions are compatible with the expectations from a thermally equilibrated source, which in addition exhibits a collective transverse expansion. However, the microscopic analyses of the transient states in the intermediate reaction stages show that the event shapes are more complex and that equilibrium is reached only in very special cases but not in event samples which cover a wide range of impact parameters as it is the case in experiments. The basic features of a new molecular dynamics model (UQMD) for heavy ion collisions from the Fermi energy regime up to the highest presently available energies are outlined.

Extracting the equation of state from a microscopic non-equilibrium model

Thu, 14 Apr 2005 14:21:32 +0200

We study the thermodynamic properties of infinite nuclear matter with the Ultrarelativistic Quantum Molecular Dynamics (URQMD), a semiclassical transport model, running in a box with periodic boundary conditions. It appears that the energy density rises faster than T4 at high temperatures of T approx. 200 - 300 MeV. This indicates an increase in the number of degrees of freedom. Moreover, We have calculated direct photon production in Pb+Pb collisions at 160 GeV/u within this model. The direct photon slope from the microscopic calculation equals that from a hydrodynamical calculation without a phase transition in the equation of state of the photon source.

Microscopic analysis of thermodynamic parameters from 160 MeV/n - 160 GeV/n

Thu, 14 Apr 2005 09:25:30 +0200

Microscopic calculations of central collisions between heavy nuclei are used to study fragment production and the creation of collective flow. It is shown that the final phase space distributions are compatible with the expectations from a thermally equilibrated source, which in addition exhibits a collective transverse expansion. However, the microscopic analyses of the transient states in the reaction stages of highest density and during the expansion show that the system does not reach global equilibrium. Even if a considerable amount of equilibration is assumed, the connection of the measurable final state to the macroscopic parameters, e.g. the temperature, of the transient ''equilibrium'' state remains ambiguous.

Reaction dynamics in Pb+Pb at the CERN/SPS: from partonic degrees of freedom to freeze-out

Wed, 13 Apr 2005 18:39:48 +0200

We analyze the reaction dynamics of central Pb+Pb collisions at 160 GeV/nucleon. First we estimate the energy density pile-up at mid-rapidity and calculate its excitation function: The energy density is decomposed into hadronic and partonic contributions. A detailed analysis of the collision dynamics in the framework of a microscopic transport model shows the importance of partonic degrees of freedom and rescattering of leading (di)quarks in the early phase of the reaction for E >= 30 GeV/nucleon. The energy density reaches up to 4 GeV/fm 3, 95% of which are contained in partonic degrees of freedom. It is shown that cells of hadronic matter, after the early reaction phase, can be viewed as nearly chemically equilibrated. This matter never exceeds energy densities of 0.4 GeV/fm 3, i.e. a density above which the notion of separated hadrons loses its meaning. The final reaction stage is analyzed in terms of hadron ratios, freeze-out distributions and a source analysis for final state pions.

Equation of state, spectra and composition of hot and dense infinite hadronic matter in a microscopic transport model

Wed, 13 Apr 2005 18:18:39 +0200

Equilibrium properties of infinite relativistic hadron matter are investigated using the Ultrarelativistic Quantum Molecular Dynamics (UrQMD) model. The simulations are performed in a box with periodic boundary conditions. Equilibration times depend critically on energy and baryon densities. Energy spectra of various hadronic species are shown to be isotropic and consistent with a single temperature in equilibrium. The variation of energy density versus temperature shows a Hagedorn-like behavior with a limiting temperature of 130 +/- 10 MeV. Comparison of abundances of different particle species to ideal hadron gas model predictions show good agreement only if detailed balance is implemented for all channels. At low energy densities, high mass resonances are not relevant; however, their importance raises with increasing energy density. The relevance of these different conceptual frameworks for any interpretation of experimental data is questioned.

Local thermodynamical equilibrium and the equation of state of hot, dense matter created in Au+Au collisions at AGS

Wed, 13 Apr 2005 18:09:34 +0200

Local kinetic and chemical equilibration is studied for Au+Au collisions at 10.7 AGeV in the microscopic Ultrarelativistic Quantum Molecular Dynamics model (UrQMD). The UrQMD model exhibits dramatic deviations from equilibrium during the high density phase of the collision. Thermal and chemical equilibration of the hadronic matter seems to be established in the later stages during a quasiisentropic expansion, observed in the central reaction cell with volume 125 fm3. For t > 10 fm/c the hadron energy spectra in the cell are nicely reproduced by Boltzmann distributions with a common rapidly dropping temperature. Hadron yields change drastically and at the late expansion stage follow closely those of an ideal gas statistical model. The equation of state seems to be simple at late times: P = 0.12 Epsilon. The time evolution of other thermodynamical variables in the cell is also presented.

Microscopic models for ultrarelativistic heavy ion collisions

Wed, 13 Apr 2005 17:48:13 +0200

In this paper, the concepts of microscopic transport theory are introduced and the features and shortcomings of the most commonly used ansatzes are discussed. In particular, the Ultrarelativistic Quantum Molecular Dynamics (UrQMD) transport model is described in great detail. Based on the same principles as QMD and RQMD, it incorporates a vastly extended collision term with full baryon-antibaryon symmetry, 55 baryon and 32 meson species. Isospin is explicitly treated for all hadrons. The range of applicability stretches from E lab < 100$ MeV/nucleon up to E lab> 200$ GeV/nucleon, allowing for a consistent calculation of excitation functions from the intermediate energy domain up to ultrarelativistic energies. The main physics topics under discussion are stopping, particle production and collective flow.

Are we close to the QGP? - Hadrochemical vs. microscopic analysis of particle production in ultrarelativistic heavy ion collisions

Wed, 13 Apr 2005 17:38:36 +0200

Ratios of hadronic abundances are analyzed for pp and nucleus-nucleus collisions at sqrt(s)=20 GeV using the microscopic transport model UrQMD. Secondary interactions significantly change the primordial hadronic cocktail of the system. A comparison to data shows a strong dependence on rapidity. Without assuming thermal and chemical equilibrium, predicted hadron yields and ratios agree with many of the data, the few observed discrepancies are discussed.