These tools will no longer be maintained as of December 31, 2024. Archived website can be found here. PubMed4Hh GitHub repository can be found here. Contact NLM Customer Service if you have questions.


BIOMARKERS

Molecular Biopsy of Human Tumors

- a resource for Precision Medicine *

119 related articles for article (PubMed ID: 34779475)

  • 41. Negative thermophoresis of nanoparticles interacting with fluids through a purely-repulsive potential.
    Tsuji T; Iseki H; Hanasaki I; Kawano S
    J Phys Condens Matter; 2017 Nov; 29(47):475101. PubMed ID: 29027907
    [TBL] [Abstract][Full Text] [Related]  

  • 42. Effect of shape anisotropy on the phase diagram of the Gay-Berne fluid.
    Mishra P; Ram J
    Eur Phys J E Soft Matter; 2005 Jul; 17(3):345-51. PubMed ID: 16007371
    [TBL] [Abstract][Full Text] [Related]  

  • 43. On the molecular origin of high-pressure effects in nanoconfinement: the role of surface chemistry and roughness.
    Long Y; Palmer JC; Coasne B; Śliwinska-Bartkowiak M; Jackson G; Müller EA; Gubbins KE
    J Chem Phys; 2013 Oct; 139(14):144701. PubMed ID: 24116635
    [TBL] [Abstract][Full Text] [Related]  

  • 44. Stability of smectic phases in the Gay-Berne model.
    de Miguel E; Martín del Río E; Blas FJ
    J Chem Phys; 2004 Dec; 121(22):11183-94. PubMed ID: 15634073
    [TBL] [Abstract][Full Text] [Related]  

  • 45. Finite-size effects in dissipative particle dynamics simulations.
    Velázquez ME; Gama-Goicochea A; González-Melchor M; Neria M; Alejandre J
    J Chem Phys; 2006 Feb; 124(8):084104. PubMed ID: 16512705
    [TBL] [Abstract][Full Text] [Related]  

  • 46. Columnar phases of discotics with orientation-dependent interactions.
    Martínez-Haya B; Cuetos A
    J Chem Phys; 2009 Aug; 131(7):074901. PubMed ID: 19708757
    [TBL] [Abstract][Full Text] [Related]  

  • 47. Effect of dispersive long-range corrections to the pressure tensor: the vapour-liquid interfacial properties of the Lennard-Jones system revisited.
    Martínez-Ruiz FJ; Blas FJ; Mendiboure B; Moreno-Ventas Bravo AI
    J Chem Phys; 2014 Nov; 141(18):184701. PubMed ID: 25399153
    [TBL] [Abstract][Full Text] [Related]  

  • 48. Equation of state and structural properties of the Weeks-Chandler-Andersen fluid.
    Heyes DM; Okumura H
    J Chem Phys; 2006 Apr; 124(16):164507. PubMed ID: 16674146
    [TBL] [Abstract][Full Text] [Related]  

  • 49. Concentration-induced planar-to-homeotropic anchoring transition of stiff ring polymers on hard walls.
    Poier P; Egorov SA; Likos CN; Blaak R
    Soft Matter; 2016 Sep; 12(38):7983-7994. PubMed ID: 27714380
    [TBL] [Abstract][Full Text] [Related]  

  • 50. Orientational order of near D(3h) solutes in nematic liquid crystals. II. Description via Gay-Berne model with embedded quadrupoles.
    Sokolovskii RO; Burnell EE
    J Chem Phys; 2009 Apr; 130(15):154507. PubMed ID: 19388759
    [TBL] [Abstract][Full Text] [Related]  

  • 51. A soft-core Gay-Berne model for the simulation of liquid crystals by Hamiltonian replica exchange.
    Berardi R; Zannoni C; Lintuvuori JS; Wilson MR
    J Chem Phys; 2009 Nov; 131(17):174107. PubMed ID: 19894998
    [TBL] [Abstract][Full Text] [Related]  

  • 52. Anisotropic behavior of organic molecules on prepatterned surfaces.
    Hopp SF; Heuer A
    J Chem Phys; 2012 Apr; 136(15):154106. PubMed ID: 22519314
    [TBL] [Abstract][Full Text] [Related]  

  • 53. Adapting SAFT-γ perturbation theory to site-based molecular dynamics simulation. III. Molecules with partial charges at bulk phases, confined geometries and interfaces.
    Ghobadi AF; Elliott JR
    J Chem Phys; 2014 Sep; 141(9):094708. PubMed ID: 25194387
    [TBL] [Abstract][Full Text] [Related]  

  • 54. Molecular dynamics simulations studies of nanoparticles in an isotropic liquid crystal matrix: Single particle behavior and pairwise interactions.
    Tian P; Smith GD; Glaser M
    J Chem Phys; 2006 Apr; 124(16):161101. PubMed ID: 16674121
    [TBL] [Abstract][Full Text] [Related]  

  • 55. Density functional theory of liquid crystals and surface anchoring: hard Gaussian overlap-sphere and hard Gaussian overlap-surface potentials.
    Avazpour A; Avazpour L
    J Chem Phys; 2010 Dec; 133(24):244701. PubMed ID: 21198002
    [TBL] [Abstract][Full Text] [Related]  

  • 56. Wetting behaviour and contact angles anisotropy of nematic nanodroplets on flat surfaces.
    Vanzo D; Ricci M; Berardi R; Zannoni C
    Soft Matter; 2016 Feb; 12(5):1610-20. PubMed ID: 26670582
    [TBL] [Abstract][Full Text] [Related]  

  • 57. A coarse-grained model of ionic liquid crystals: the effect of stoichiometry on the stability of the ionic nematic phase.
    Saielli G; Satoh K
    Phys Chem Chem Phys; 2019 Sep; 21(36):20327-20337. PubMed ID: 31495845
    [TBL] [Abstract][Full Text] [Related]  

  • 58. Comparison of the capillary wave method and pressure tensor route for calculation of interfacial tension in molecular dynamics simulations.
    Nickerson S; Frost DS; Phelan H; Dai LL
    J Comput Chem; 2013 Dec; 34(31):2707-15. PubMed ID: 24122780
    [TBL] [Abstract][Full Text] [Related]  

  • 59. The line tension of two-dimensional ionic fluids.
    Eustaquio-Armenta Mdel R; Méndez-Maldonado GA; González-Melchor M
    J Chem Phys; 2016 Apr; 144(13):134705. PubMed ID: 27059583
    [TBL] [Abstract][Full Text] [Related]  

  • 60. Monte Carlo simulation of two-dimensional hard rectangles: confinement effects.
    Triplett DA; Fichthorn KA
    Phys Rev E Stat Nonlin Soft Matter Phys; 2008 Jan; 77(1 Pt 1):011707. PubMed ID: 18351866
    [TBL] [Abstract][Full Text] [Related]  

    [Previous]   [Next]    [New Search]
    of 6.