Semiconductor nanocrystals are a promising class of materials for a variety of novel optoelectronic devices, since many of their properties, such as the electronic gap and conductivity, can be controlled. Much of this control is achieved via the organic ligand shell, through control of the size of the nanocrystal and the distance to other objects. We here simulate ligand-coated CdSe nanocrystals using atomistic molecular dynamics, allowing for the resolution of novel structural details about the ligand shell. We show that the ligands on the surface can lie flat to form a highly anisotropic 'wet hair' layer as opposed to the 'spiky ball' appearance typically considered.We discuss how this can give rise to a dot-to-dot packing distance of one ligand length since the thickness of the ligand shell is reduced to approximately one-half of the ligand length for the system sizes considered here; these distances imply that energy and charge transfer rates between dots and nearby objects will be enhanced due to the thinner than expected ligand shell. Our model predicts a non-linear scaling of ligand shell thickness as the ligands transition from 'spiky' to 'wet hair'. We verify this scaling using TEM on a PbS nanoarray, confirming that this theory gives a qualitatively correct picture of the ligand shell thickness of colloidal quantum dots. * tvan@mit.edu 1 arXiv:1706.00844v1 [physics.chem-ph] 2 Jun 2017 Semiconducting quantum dots have attracted substantial attention due to their tunable structure-property relationships [1][2][3][4][5][6]. The ability to simultaneously engineer their electronic and optical properties within a single device has made them a prime candidate material in a variety of applications. In solar cells and LEDs, quantum dot size is used to tune band gaps, and this is commonly exploited to produce varied spectral properties [7][8][9][10][11].These optoelectronic devices function through electronic processes that are often strongly dependent on distance [5,[12][13][14][15]. For example, conductivity in a quantum dot array is mediated by Marcus-type charge transfer events between dots [9,13,[16][17][18][19][20][21][22]. As the dot-todot distance increases, the charge transfer rate decays exponentially, making the conductivity extremely sensitive to the dot-to-dot distance [16,17,23,24]. Excitonic energy transfer, relevant in solar cells and light emitters, usually occurs through Forster resonant energy transfer (FRET) [1,21,[25][26][27][28][29][30] or Dexter processes [31][32][33]; these are also dependent on distance. Since the organic ligand shell is usually composed of insulating alkane chains, they behave as a spacer layer that can determine that closest approach distance [13,[19][20][21]34].Ligand exchange reactions [35][36][37][38] give us in situ synthetic access to the ligand shell, and using this design space it is possible to achieve fine control of the aforementioned electronic processes.Recently, the ability to control the energy gap and energy transfer has been exploited for novel optoelect...