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Recombination Losses (recombination + loss)

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Physics and Astronomy	33%

Selected Abstracts

Estimates of genetic parameters for Boran, Friesian, and crosses of Friesian and Jersey with the Boran cattle in the tropical highlands of Ethiopia: milk production traits and cow weight

JOURNAL OF ANIMAL BREEDING AND GENETICS, Issue 3 2004
S. Demeke
Summary Breed additive and non-additive effects plus heritabilities and repeatabilities for milk yield per lactation (LMY), milk yield per day (DMY), lactation length (LL), annual milk yield (AMY), annual milk yield per metabolic body weight (AMYBW) and cow weight at calving (BW) were estimated for 5464 lactation records collected from purebred Boran (B), Friesian (F), and crosses of Friesian and Jersey (J) breeds with the Boran breed raised in the tropical highlands of Ethiopia. Single trait analysis was carried out by using two equivalent repeatability animal models. In the first model the genotype was fitted as a fixed group effect, while in the second model the genotype was substituted by breed additive, heterotic and recombination effects fitted as fixed covariates. Both the F and J breed additive effects, measured as a deviation from the B breed were significant (p < 0.01) for all traits, except for BW of the J. The F and J additive contributions were 2774 ± 81 and 1473 ± 362 kg for LMY, 7.1 ± 0.2 and 4.8 ± 0.8 kg for DMY, 152 ± 7 and 146 ± 31 days for LL, 2345 ± 71 and 1238 ± 319 kg for AMY, 20.6 ± 0.9 and 18.9 ± 4.3 kg for AMYBW, and 140 ± 4 and ,21 ± 22 kg (p > 0.05) for BW. The heterotic contributions to the crossbred performance were also positive and significant (p < 0.01) for all traits. The F1 heterosis expressed as a deviation from the mid-parent values were 22 and 66% for LMY, 11 and 20% for DMY, 29 and 29% for LL, 21 and 64% for AMY, 42 and 42% for AMYBW, and 2% (p < 0.05) and 11% for BW for the F × B and J × B crosses, respectively. The recombination effect estimated for the F × B crosses was negative and significant for LMY (,526 ± 192 kg, p < 0.01), DMY (,3.0 ± 0.4 kg, p < 0.001), AMY (,349 ± 174 kg, p < 0.05) and BW (,68 ± 11 kg, p < 0.001). For the J × B crosses the recombination loss was significant and negative only for DMY (,2.2 ± 0.7 kg, p < 0.05) and BW (,33 ± 17 kg, p < 0.05). The direct heritabilities (h2) estimated for LMY, DMY, LL, AMY and AMYBW were 0.24 ± 0.04, 0.19 ± 0.03, 0.13 ± 0.03, 0.23 ± 0.04 and 0.17 ± 0.05, respectively. Based on the genetic parameters estimated, the best breeding strategy to increased milk production under highland Ethiopian conditions is to apply selection on purebred base populations (Boran and Friesian) and then crossing them to produce F1 dairy cows. However, for breeding decision based on total dairy merit, further investigations are needed for traits such as milk quality, reproduction, longevity and survival. Zusammenfassung Additive Rasseneffekte, nicht additive Effekte, Heritabilitäten und Wiederholbarkeiten für Milchmenge pro Laktation (LMY), Milchmenge pro Tag (DMY), Laktationsdauer (LL), jährliche Milchmenge (AMY), jährliche Milchmenge pro metabolischem Körpergewicht (AMYBW) und Kuhgewichte zur Kalbung (BW) wurden anhand von 5464 Laktationsdatensätzen von reinrassigen Boran (B), Friesian (F) und Kreuzungen der Rassen Friesian und Jersey (J) mit der Rasse Boran, die im tropischen Hochland von Äthiopien groß gezogen wurden, geschätzt. Einmerkmalsmodelle wurden mit zwei äquivalenten Wiederholbarkeits-Tiermodellen durchgeführt. Im ersten Modell wurde der Genotyp als fixer Gruppeneffekt berücksichtigt, während im zweiten Modell der Genotyp durch additive Rasseneffekte, Heterosis und Rekombinationseffekte als Kovariable ersetzt wurde. Die additiven Rasseneffekte von F und J, gemessen als Abweichung von der Rasse B, waren für alle Merkmale signifikant (p < 0,01), ausgenommen BW für die Rasse J. Die additiven Rasseneffekte von F und J betrugen 2774 ± 81 und 1473 ± 362 kg für LMY, 7,1 ± 0,2 und 4,8 ± 0,8 kg für DMY, 152 ± 7 und 146 ± 31 Tage für LL, 2345 ± 71 und 1238 ± 319 kg für AMY, 20,6 ± 0,9 und 18,9 ± 4,3 kg für AMYBW und 140 ± 4 und ,21 ± 22 kg (p > 0,05) für BW. Die Heterosis bei den Kreuzungstieren war positiv und signifikant für alle Merkmale (p < 0,01). Die Heterosis der F1 -Tiere, ausgedrückt als Abweichung vom Mittel der beiden Eltern, betrug 22 und 66% für LMY, 11 und 20% für DMY, 29 und 29% für LL, 21 und 64% für AMY, 42% und 42% für AMYBW und 2% (p < 0,05) und 11% für BW für die F × B und J × B Kreuzungen. Der geschätzte Rekombinationseffekt für die F × B Kreuzungen war negativ und signifikant für LMY (,526 ± 192 kg, p < 0,01), DMY (,3,0 ± 0,4 kg, p < 0,001), AMY (,349 ± 174, p < 0,05) und BW (,68 ± 11 kg, p < 0,001). Für die J × B Kreuzungen war der Rekombinationsverlust signifikant und negativ nur für DMY (,2,2 ± 0,7 kg, p < 0,05) und BW (,33 ± 17, p < 0,05). Die geschätzten Heritabilitäten (h2) betrugen für LMY, DMY, LL, AMY und AMYBW 0,24 ± 0,04, 0,19 ± 0,03, 0,13 ± 0,03, 0,23 ± 0,04 und 0,17 ± 0,05. Basierend auf den geschätzten genetischen Parametern erscheint Selektion in den Reinzuchtpopulationen B und F und anschließ end Kreuzung dieser Tiere zur Erstellung von F1 -Milchkühen als günstigste Zuchtstrategie, um die Milchproduktion unter äthiopischen Hochlandbedingungen zu steigern. Für Zuchtentscheidungen, die die gesamte Milchproduktion berücksichtigen, sind weitere Untersuchungen notwendig für Merkmale wie Milchqualität, Reproduktion, Persistenz und Langlebigkeit. [source]

Origin of the Reduced Fill Factor and Photocurrent in MDMO-PPV:PCNEPV All-Polymer Solar Cells,

ADVANCED FUNCTIONAL MATERIALS, Issue 13 2007
M. Mandoc
Abstract The photogeneration mechanism in blends of poly[2-methoxy-5-(3,,7,-dimethyloctyloxy)-1,4 - phenylene vinylene] (MDMO-PPV) and poly[oxa-1,4-phenylene-(1-cyano-1,2-vinylene)-(2-methoxy-5-(3,,7,-dimethyloctyloxy)-1,4-phenylene)-1,2-(2-cyanovinylene)-1,4-phenylene] (PCNEPV) is investigated. The photocurrent in the MDMO-PPV:PCNEPV blends is strongly dependent on the applied voltage as a result of a low dissociation efficiency of the bound electron,hole pairs. The dissociation efficiency is limited by low carrier mobilities, low dielectric constant, and the strong intermixing of the polymers, leading to a low fill factor and a reduced photocurrent at operating conditions. Additionally, electrons trapped in the PCNEPV phase recombine with the mobile holes in the MDMO-PPV phase at the interface between the two polymers, thereby affecting the open-circuit voltage and increasing the recombination losses. At an intensity of one,sun, Langevin recombination of mobile carriers dominates over trap-assisted recombination. [source]

Influence of charge carrier mobility on the performance of organic solar cells

PHYSICA STATUS SOLIDI - RAPID RESEARCH LETTERS, Issue 4 2008
Carsten Deibel
Abstract The power conversion efficiency of organic solar cells based on donor,acceptor blends is governed by an interplay of polaron pair dissociation and bimolecular polaron recombination. Both processes are strongly dependent on the charge carrier mobility, the dissociation increasing with faster charge transport, with raised recombination losses at the same time. Using a macroscopic effective medium simulation, we calculate the optimum charge carrier mobility for the highest power conversion efficiency, for the first time accounting for injection barriers and a reduced Langevin-type recombination. An enhancement of the charge carrier mobility from 10,8 m2/V s for state of the art polymer,fullerene solar cells to about 10,6 m2/V s, which yields the maximum efficiency, corresponds to an improvement of only about 20% for the given parameter set. (© 2008 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim) [source]

Light trapping in organic solar cells

PHYSICA STATUS SOLIDI (A) APPLICATIONS AND MATERIALS SCIENCE, Issue 12 2008
Michael Niggemann
Abstract One key problem in optimizing organic solar cells is to maximize the absorption of incident light and to keep the charge carrier transport paths as short as possible in order to minimize recombination losses during the charge carrier extraction. The large versatility of organic semiconductors and compositions requires specific optimization of each system. Due to the small thickness of the functional layers in the order of several ten nanometres, coherent optics has to be considered and therefore interference effects play a dominant role. Here we present and discuss concepts for light trapping in organic solar cells. These are wide gap layers in planar solar cells, folded solar cell architectures benefiting from the illumination under inclined incident angles and multiple reflections and absorptions as well as diffraction gratings embossed into the photoactive layer. (© 2008 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim) [source]

Spatially resolved evaluation of power losses in industrial solar cells by illuminated lock-in thermography

PROGRESS IN PHOTOVOLTAICS: RESEARCH & APPLICATIONS, Issue 5 2004
Joerg Isenberg
Abstract The principles of a recently introduced measurement technique for power losses in solar cells, illuminated lock-in thermography (ILT), are reviewed. The main advantage of ILT over dark lock-in Thermography (DLT) is measurement under realistic operational conditions of solar cells. The main focus of this paper is to demonstrate the wide range of applications of ILT in identifying the causes of power losses in solar cells. For this purpose different evaluation methods are presented. A method for the evaluation of improvement potentials within a given cell technology is demonstrated. It is shown that different types of series resistance may be localized. Small areas of recombination losses (e.g., grain boundaries) can routinely be detected, which is not possible in dark lock-in thermography. Good correspondence with light-beam-induced current images is found. A realistic evaluation of the impact of recombination losses on solar cell performance is demonstrated on two examples. Finally, process- or treatment-induced recombination losses are investigated. In summary ILT is shown to be an extremely powerful tool in localizing, identifying and quantifying power losses of solar cells under realistic illumination conditions. Copyright © 2004 John Wiley & Sons, Ltd. [source]

Advances in Photoelectrocatalysis with Nanotopographical Photoelectrodes

CHEMPHYSCHEM, Issue 8 2010
A. G. Muñoz Dr.
Abstract The design of photoelectrodes for high efficiency solar fuel energy conversion devices is based on the search for adequate surface conditioning to achieve efficient light harvesting, stability, minimized surface recombination losses and high electron-transfer rates at the electrolyte interface. An overview on established and novel approaches is given. A recent viable solution is provided by electroplating of nanoscale catalytic metals on passivated semiconductor surfaces, thereby forming reactive centers and avoiding contact between the semiconductor surface and the electrolyte. At these nano-dimensioned Schottky-type junctions, light-induced excess minority carriers are scavenged and transferred to the electrolyte. Various possible device configurations are outlined and envisaged systems for hydrogen or oxygen evolution and carbon dioxide reduction are presented. The role of ultrathin passivating films is emphasized and methods to fabricate open as well as compact conformal films are described. [source]