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1.
Anim Genet ; 52(5): 645-655, 2021 Oct.
Article in English | MEDLINE | ID: mdl-34324723

ABSTRACT

lncRNAs play crucial roles in fat metabolism in animals. Previously, we have compared the mRNA transcriptome profiles between seven fat-type Chinese pig breeds and one lean-type Western breed (Yorkshire, YY). The associations between differentially expressed (DE) genes and phenotypical traits were investigated. In the present study, to further explore the underlying regulatory mechanisms, lncRNAs were sequenced and compared between YY and Chinese indigenous breeds. The results showed 9114 and 7538 DE lncRNAs between at least one Chinese breed and the YY breed in the adipose and muscle tissue respectively. KEGG enrichment analysis revealed that the target genes of these DE lncRNAs mainly influenced the glucolipid metabolism, which is an important process affecting meat quality. Correlation analyses between the DE lncRNA and DE mRNA genes related to meat quality and growth traits were performed. The results showed that LTCONS_00073280 was associated with intramuscular fat content. Four lncRNAs (LTCONS_00101781, LTCONS_00037879, LTCONS_00088260 and LTCONS-00128343) might mediate backfat thickness. Overall, this study provides candidate lncRNAs that potentially affect meat quality, which might be useful for molecular breeding of pig breeds in future.


Subject(s)
Adipose Tissue , Muscles , RNA, Long Noncoding/genetics , Sus scrofa/genetics , Animals , Breeding , Phenotype , Pork Meat
2.
J Chem Phys ; 144(17): 174703, 2016 May 07.
Article in English | MEDLINE | ID: mdl-27155643

ABSTRACT

A comprehensive study is presented for the influence of misfit strain, adhesion strength, and lattice symmetry on the complex Moiré patterns that form in ultrathin films of honeycomb symmetry adsorbed on compact triangular or honeycomb substrates. The method used is based on a complex Ginzburg-Landau model of the film that incorporates elastic strain energy and dislocations. The results indicate that different symmetries of the heteroepitaxial systems lead to distinct types of domain wall networks and phase transitions among various surface Moiré patterns and superstructures. More specifically, the results show a dramatic difference between the phase diagrams that emerge when a honeycomb film is adsorbed on substrates of honeycomb versus triangular symmetry. It is also shown that in the small deformation limit, the complex Ginzburg-Landau model reduces to a two-dimensional sine-Gordon free energy form. This free energy can be solved exactly for one dimensional patterns and reveals the role of domains walls and their crossings in determining the nature of the phase diagrams.

3.
Phys Rev Lett ; 108(22): 226102, 2012 Jun 01.
Article in English | MEDLINE | ID: mdl-23003626

ABSTRACT

Thin heteroepitaxial overlayers have been proposed as templates to generate stable, self-organized nanostructures at large length scales, with a variety of important technological applications. However, modeling strain-driven self-organization is a formidable challenge due to different length scales involved. In this Letter, we present a method for predicting the patterning of ultrathin films on micron length scales with atomic resolution. We make quantitative predictions for the type of superstructures (stripes, honeycomb, triangular) and length scale of pattern formation of two metal-metal systems, Cu on Ru(0001) and Cu on Pd(111). Our findings are in excellent agreement with previous experiments and call for future experimental investigations of such systems.

4.
Eur Phys J E Soft Matter ; 29(4): 423-9, 2009 Aug.
Article in English | MEDLINE | ID: mdl-19669181

ABSTRACT

We investigate several properties of a translocating homopolymer through a thin pore driven by an external field present inside the pore only using Langevin Dynamics (LD) simulations in three dimensions (3D). Motivated by several recent theoretical and numerical studies that are apparently at odds with each other, we estimate the exponents describing the scaling with chain length (N) of the average translocation time , the average velocity of the center of mass , and the effective radius of gyration during the translocation process defined as approximately Nalpha, approximately N(-delta), and Rg approximately Nnu respectively, and the exponent of the translocation coordinate (s-coordinate) as a function of the translocation time approximately tbeta. We find alpha = 1.36 +/- 0.01, beta = 1.60+/- 0.01 for approximately taubeta and beta = 1.44 +/- 0.02 for approximately taubeta, delta = 0.81 +/- 0.04, and nu congruent with nu = 0.59 +/- 0.01, where nu is the equilibrium Flory exponent in 3D. Therefore, we find that approximately N1.36 is consistent with the estimate of approximately /. However, as observed previously in Monte Carlo (MC) calculations by Kantor and Kardar (Y. Kantor, M. Kardar, Phys. Rev. E 69, 021806 (2004)) we also find the exponent alpha = 1.36 +/- 0.01 < 1 + nu. Further, we find that the parallel and perpendicular components of the gyration radii, where one considers the "cis" and "trans" parts of the chain separately, exhibit distinct out-of-equilibrium effects. We also discuss the dependence of the effective exponents on the pore geometry for the range of N studied here.


Subject(s)
Motion , Nanostructures/chemistry , Polymers/chemistry , Models, Chemical , Models, Molecular , Porosity , Time Factors
5.
Eur Phys J E Soft Matter ; 28(4): 385-93, 2009 Apr.
Article in English | MEDLINE | ID: mdl-19326157

ABSTRACT

Using Langevin dynamics simulations, we investigate the translocation dynamics of an externally driven polymer chain through a nanopore, where a pulling force F is exerted on the first monomer whilst there is an opposing force F(E) < F within the pore. Such a double-force arrangement has been proposed recently to allow better dynamical control of the translocation process in order to sequence biopolymers. We find that in the double-force arrangement translocation becomes slower as compared to the case under a single monomer pulling force of magnitude F-F(E), but scaling of the translocation time as a function of the chain length tau approximately N2 does not change. The waiting time tau(m) for monomer m to exit the pore is found to be a monotonically increasing function of the bead number almost until m approximately N , which indicates relatively well-defined slowing down and control of the chain velocity during translocation. We also study the waiting time distributions for the beads in the chain, and characterize in detail fluctuations in the bead positions and their transverse position coordinates during translocation. These data should be useful in estimating position-dependent sequencing errors in double-force experiments.


Subject(s)
Biopolymers/metabolism , Biological Transport , Computer Simulation , DNA, Single-Stranded/chemistry , DNA, Single-Stranded/metabolism , Models, Biological , Nanotechnology , Nucleotides/metabolism , Porosity , Time Factors
6.
Phys Rev B Condens Matter ; 54(12): 8856-8861, 1996 Sep 15.
Article in English | MEDLINE | ID: mdl-9984567
8.
Phys Rev Lett ; 73(5): 700-703, 1994 Aug 01.
Article in English | MEDLINE | ID: mdl-10057515
9.
Phys Rev B Condens Matter ; 49(19): 13838-13847, 1994 May 15.
Article in English | MEDLINE | ID: mdl-10010331
10.
Phys Rev Lett ; 71(26): 4361-4364, 1993 Dec 27.
Article in English | MEDLINE | ID: mdl-10055227
11.
Phys Rev B Condens Matter ; 48(19): 14524-14528, 1993 Nov 15.
Article in English | MEDLINE | ID: mdl-10007874
12.
Phys Rev B Condens Matter ; 48(8): 5679-5681, 1993 Aug 15.
Article in English | MEDLINE | ID: mdl-10009093
13.
Phys Rev B Condens Matter ; 47(4): 2333-2343, 1993 Jan 15.
Article in English | MEDLINE | ID: mdl-10006274
14.
15.
Phys Rev Lett ; 68(12): 1866-1868, 1992 Mar 23.
Article in English | MEDLINE | ID: mdl-10045240
17.
19.
Phys Rev B Condens Matter ; 43(15): 12234-12245, 1991 May 15.
Article in English | MEDLINE | ID: mdl-9997020
20.
Phys Rev B Condens Matter ; 42(16): 10264-10274, 1990 Dec 01.
Article in English | MEDLINE | ID: mdl-9995286
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