Their intrinsically high k is due to high electrical conductivity or harmonic crystal lattices. [10][11][12] Organic polymers are considered poor thermal conductors due to their randomly coiled covalent backbone and poor electrical conductivity, with low thermal conductivities on the order of 0.1 W m −1 K −1 . [13] However, early studies achieved orders of magnitude increases in k in oriented single chains, crystals, and anisotropic polymers, such as polyethylene (PE), poly(p-phenylene benzobisoxazole) (PBO), polythiophene, and Kevlar. [14][15][16] This creates opportunities to synthesize inexpensive, lightweight and electrically insulating thermal conductors to replace traditional metals and ceramics in specific applications.Taking the simplest polymer, PE, as an example, the milestone work was carried out by Choy et al., [17,18] where PE crystallites with a folded carbon-carbon backbone were restructured via extrusion to perform a large anisotropy in k. Since then, a variety of high-k products have been reported, including fibers, films, and bulks. [19][20][21][22][23][24][25] For instance, a high-k PE mat containing a large number of needle crystals was prepared that exhibited an axial k of 41.8 W m −1 K −1 , [26] about three times higher than steel; recently, this value has been further extended to 62 W m −1 K −1 in a PE thin-film through a typical disentanglement-extrusion-freezing process. [25] Shen et al. converted ultra-drawn PE objects into ideal single-crystalline nanofibers, achieving a record-high k of 104 W m −1 K −1 in the fiber direction. [19] Our lab previously took advantage of high-k PE microfibers to design an entirely organic and large-thickness bulk, exhibiting a k as high as 38.27 W m −1 K −1 in the through-plane direction. [27] Two conflicting explanations have been postulated for the efficient thermal transport in oriented polymers: one theorizes that content increment and/or dimension enlargement of the fibrillar crystal cause the remarkable thermal conduction; [23] the other attributes this to the evolving high k in the amorphous phase during the orientation process, for example, a classic 1D model calculated the k of amorphous domain in an ultra-drawn PE film to be as high as 16 W m −1 K −1 . [25] The high-k nature of polymers requires further experimental support and mechanistic explanations. Additionally, the highly thermal conductive characteristic for current polymer samples is still limited to only one specific direction, e.g., the axial direction for fibers and in-plane direction for films. 3D high thermal Polymers are usually considered thermal insulators; however, significant enhancements in thermal conductivity (k) have been observed in oriented fibers and films. Despite being advantageous in real-world applications, extending the linear thermal-transport advantage of polymers into the 3D space in bulk materials is still limited due to the spatially interfacial phononconduction barriers. Herein, inspired by the structure of tropocollagen, it is discovered that weaving hierarchi...