Spin current has emerged as a leading candidate for manipulation of spins in a nanomagnet. We here experimentally show another utility of spin current viz. it can be used for generation of phonons. Within the same experimental setup, we also demonstrate the inverse effect of generation of spin current by phonons. To demonstrate them, we measured the scattering-matrix of a two-port device with interdigital transducers as one port and array of Ni/Pt lines as second port on piezoelectric substrate. The off-diagonal elements which correspond to transmission between the ports, were found to have 180 o relative phase shift. The transmission of electrical signal from port 2 to 1 corresponds to generation of phonons from spin-current, while transmission from port 1 to 2 corresponds to the inverse effect. These results could be useful for designing spin-current based gyrators.Spintronics exploits the spin degree of freedom of an electron for various new functionalities [1]. The coupling of spins to heat currents (spin caloritronics) [2-9] orbital momentum (spin orbitronics) [10][11][12][13] or the mechanical degrees of freedom (spin mechanics) [14][15][16][17][18][19][20][21][22] has generated a lot of interest due to the novel physics involved and potential new applications of spin current. This coupling has enabled observation of various new phenomena such as spin Seebeck effect [3][4][5][6], acoustically driven resonance [15][16][17] etc. Spin seebeck effect refers to the generation of spin current over a macroscopic scale by temperature gradient, whereas in acoustically driven resonance, mechanical motion is used to excite spin dynamics. We here demonstrate that spin current can be used to excite phonons, which can travel macroscopic distances of the order of millimeter. Our experiment utilizes a piezoelectric LiNbO 3 substrate over which we fabricate a periodic array of Ni/Pt lines. We observed that when current is passed through Ni/Pt lines, phonons in the form of surface acoustic waves (SAW) are emitted, which can be detected by using interdigital transducers (IDT). This phonon emission involves many spin based phenomena: i) Conversion of charge current into spin current by spin-Hall effect (SHE) in Pt ii) Excitation of magnons in Ni by spin current via spin-transfer torque (STT) effect iii) emission of phonons by magnons via magneto-elastic coupling. Our setup also allows us to measure the inverse effect i.e. generation of spin current by phonons [19]. The inverse effect proceeds via inverse of the above three steps: i) generation of magnons by phonons via inverse magneto-elastic coupling ii) injection of spin current in Pt via. inverse STT effect or spin pumping iii) Conversion of spin current into charge current by inverse spin-Hall effect (ISHE) in Pt.Our experiments show that the transmission of electrical signal from IDTs to Ni/Pt lines (S 21 ) and transmission from Ni/Pt lines to IDTs (S 12 ) have opposite sign i.e. S 12 =-S 21 i.e. the
Corresponding Author* Email: ashwin@ee.iitb.ac.in
Author ContributionsTh...