[1] H. Salman (2014): A time-splitting pseudospectral method for the solution of the Gross-Pitaevskii equations using spherical harmonics with generalised-Laguerre basis functions,  Journal of Computational Physics, 258, 185-207.

[2] H. Salman (2013): Breathers on quantized superfluid vortices Physical Review Letters (PRL), 111, 165301.

[3] H. Salman, N.G. Berloff, P.H. Roberts (2013): From Classical Fields to Two-Fluid Model of Superfluidity: Emergent Kinetics and Local Gauge Transformationsin Quantum Gases: Finite Temperatures and Non-Equilibrium Dynamics. , eds. M. Davis, S. Gardiner, N. Nygaard, N. Proukakis, and M. Szymanska, World Scientific, 369-384.

[4] H. Salman (2012): Approximating steady states in equilibrium and nonequilibrium condensatesPhysical Review A (PRA), 85, 063622.

[5] H. Salman and N.G. Berloff, (2009): Condensation  of classical nonlinear waves in a two-component systemPhysica D, 238, 1482-1489.

[6] H. Salman, (2008): Hybrid Grid/Particle Filter for Lagrangian  Data Assimilation. Part I: Formulating the passive scalar approximation, Q. J. Roy. Meteor. Soc., 134, 1539-1550.

[7] H. Salman, (2008): A Hybrid Grid/Particle Filter for Lagrangian Data Assimilation. Part II: Application to a model vortex flowQ. J. Roy. Meteor. Soc., 134, 1551-1565.

[8] H. Salman, K. Ide, and C.K.R.T. Jones, (2008): Using Flow Geometry for Drifter Deployment in Lagrangian Data AssimilationTellus A., 60, 336-347. 

[9] H. Salman and P.H. Haynes, (2007): A Numerical Study of Passive Scalar Evolution in Peripheral Regions, Phys. Fluids., 19, 067101 1-20.

[10] H. Salman, J.S. Hesthaven, T. Warburton, and G. Haller, (2007): Predicting Transport by Lagrangian Coherent Structures with a High Order Method, Theor. Comp. Fluid Dyn., 21, 39-58.

[11] H. Salman, L. Kuznetsov, C.K.R.T. Jones, and K. Ide, (2006): A Method for Assimilating Lagrangian Data into a Shallow-Water Equation Ocean Model, Mon. Weather Rev., 134, 1081-1101.

[12] H. Salman, J.J. McGuirk, and G.J. Page, (2006): Prediction of a 3D non-isothermal mixing layer created by a scarfed lobed mixer, Proceedings of the IMECHE Part G - Journal of Aerospace Engineering, 220, 399-419.

[13] H. Salman, and M. Soteriou, (2004): Lagrangian simulation of evaporating droplet spraysPhys. Fluids., 16, 4601-4622.

[14] H. Salman, D. Jiang, J.J. McGuirk, and G.J. Page, (2004): Linear and non-linear turbulence model predictions of vortical flows in lobed mixers, Aeronautical Journal, 108, 65--73.

[15] H. Salman, G.J. Page, and J.J. McGuirk, (2003): Prediction of lobed mixer vortical structures with a k-epsilon turbulence model, AIAA Journal., 41, 878-887.

[16] G. Haller, Y. Wang, H. Salman, J.S. Hesthaven, A. Banaszuk, (2002): Control of Lagrangian Coherent Structures, IUTAM Symposium on Unsteady Separated Flows, April 8-12, Toulouse, France.

[17] H. Salman, J.J. McGuirk, G.J. Page, and P. Moinier, (2000): The influence of unstructured mesh type on the prediction of convoluted shear layers, ECCOMAS, Barcelona, Spain.

[18] H. Salman, J.J. McGuirk, and G.J. Page, (1999): A numerical study of vortex interactions in lobed mixer flow fields , AIAA 30th Fluid Dynamics Conference, AIAA Paper 99-3409, Norfolk, VA, USA.