We have performed polarized Raman scattering measurements on WTe2, for which an extremely large positive magnetoresistance has been reported recently. We observe 5 A1 phonon modes and 2 A2 phonon modes out of 33 Raman active modes, with frequencies in good accordance with firstprinciples calculations. The angular dependence of the intensity of the peaks observed is consistent with the Raman tensors of the C2v point group symmetry attributed to WTe2. Although the phonon spectra suggest neither strong electron-phonon nor spin-phonon coupling, the intensity of the A1 phonon mode at 160.6 cm −1 shows an unconventional decrease with temperature decreasing, for which the origin remains unclear.PACS numbers: 74.70. Xa, 75.47.De, 74.25.Kc Giant magnetoresistance is at the core of several important applications, notably for the storage of information. The recent discovery of extremely large positive magnetoresistance (XMR) in layered WTe 2 [1] triggered sudden interest for this material. In particular, the nonsaturating XMR in WTe 2 has been attributed to perfectly balanced electron-hole populations [1,2], similar as in pure bismuth and graphite [3,4]. Interestingly, this effect is strongly affected by external pressure [5], and pressure-induced superconductivity has even been reported [6,7], which questions the importance of the interactions between the electronic structure and the lattice in WTe 2 , and offers additional possibilities for development of devices. Unfortunately, literature still lacks of report on the dynamical properties of the lattice in this system.In this letter, we use Raman scattering spectroscopy to characterize the phonons of WTe 2 single-crystals. We observe 7 out of 33 Raman active modes, with frequencies in good accordance with our first-principles calculations. The angular dependence of the Raman intensity of these modes is consistent with their symmetry assignments in terms of the C 2v point group symmetry of WTe 2 . In contrast to our expectation, none of the phonons observed shows evidence for an electron-phonon coupling. However, the intensity of a A 1 phonon peak at 160.6 cm −1 exhibits an unusual decrease upon cooling, whose origin remains unclear.The WTe 2 single crystals used in our Raman scattering measurements were grown by solid-state reactions. The resistivity of the samples was measured with a Quantum Design physical properties measurement system (PPMS). The crystals were cleaved in air to obtain flat surfaces and then transferred into a low-temperature cryostat ST500 (Janis) for the Raman measurements between 5 and 300 * These two authors contributed equally to this work.† p.richard@iphy.ac.cn ‡ dingh@iphy.ac.cn K with a working vacuum better than 8 × 10 −7 mbar. Raman scattering measurements were performed using a 514.5 nm excitation laser in a back-scattering microRaman configuration, with a triple-grating spectrometer (Horiba Jobin Yvon T64000) equipped with a nitrogencooled CCD camera. In this manuscript, we define x and y as the directions along the a axis (W-W chains) a...