Maxim Goryachev
University of Western Australia
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Publication
Featured researches published by Maxim Goryachev.
Physical review applied | 2014
Maxim Goryachev; Warrick G. Farr; Daniel L. Creedon; Yaohui Fan; Mikhail Kostylev; Michael E. Tobar
Using a sub-millimetre sized YIG (Yttrium Iron Garnet) sphere mounted in a magnetic field-focusing cavity, we demonstrate an ultra-high cooperativity of
Applied Physics Letters | 2012
Maxim Goryachev; Daniel L. Creedon; Eugene Ivanov; Serge Galliou; Roger Bourquin; Michael E. Tobar
10^5
Scientific Reports | 2013
Serge Galliou; Maxim Goryachev; Roger Bourquin; Philippe Abbé; Michael E. Tobar
between magnon and photon modes at millikelvin temperatures and microwave frequencies. The cavity is designed to act as a magnetic dipole by using a novel multiple-post approach, effectively focusing the cavity magnetic field within the YIG crystal with a filling factor of 3%. Coupling strength (normal-mode splitting) of 2 GHz, (equivalent to 76 cavity linewidths or
Physical Review Letters | 2013
Maxim Goryachev; Daniel L. Creedon; Serge Galliou; Michael E. Tobar
0.3
Applied Physics Letters | 2011
Serge Galliou; J. Imbaud; Maxim Goryachev; Roger Bourquin; Philippe Abbé
Hz per spin), is achieved for a bright cavity mode that constitutes about 10% of the photon energy and shows that ultra-strong coupling is possible in spin systems at microwave frequencies. With straight forward optimisations we demonstrate that with that this system has the potential to reach cooperativities of
Physical Review B | 2015
Daniel L. Creedon; Jean-Michel Le Floch; Maxim Goryachev; Warrick G. Farr; Stefania Castelletto; Michael E. Tobar
10^7
Physical Review B | 2016
Jeremy Bourhill; Nikita Kostylev; Maxim Goryachev; Daniel L. Creedon; Michael E. Tobar
, corresponding to a normal mode splitting of 5.2 GHz and a coupling per spin approaching 1 Hz. We also observe a three-mode strong coupling regime between a dark cavity mode and a magnon mode doublet pair, where the photon-magnon and magnon-magnon couplings (normal-mode splittings) are 143 MHz and 12.5 MHz respectively, with HWHM bandwidth of about 0.5 MHz.
Physical Review D | 2014
Maxim Goryachev; Michael E. Tobar
Low-loss, high frequency acoustic resonators cooled to millikelvin temperatures are a topic of great interest for application to hybrid quantum systems. When cooled to 20 mK, we show that resonant acoustic phonon modes in a bulk acoustic wave quartz resonator demonstrate exceptionally low loss (with Q-factors of order billions) at frequencies of 15.6 and 65.4 MHz, with a maximum f · Q product of 7.8 × 1016 Hz. Given this result, we show that the Q-factor in such devices near the quantum ground state can be four orders of magnitude better than previously attained. Such resonators possess the low losses crucial for electromagnetic cooling to the phonon ground state, and the possibility of long coherence and interaction times of a few seconds, allowing multiple quantum gate operations.Low-loss, high frequency acoustic resonators cooled to millikelvin temperatures are a topic of great interest for application to hybrid quantum systems. When cooled to 20 mK, we show that resonant acoustic phonon modes in a bulk acoustic wave quartz resonator demonstrate exceptionally low loss (with Q-factors of order billions) at frequencies of 15.6 and 65.4 MHz, with a maximum f · Q product of 7.8 × 1016 Hz. Given this result, we show that the Q-factor in such devices near the quantum ground state can be four orders of magnitude better than previously attained. Such resonators possess the low losses crucial for electromagnetic cooling to the phonon ground state, and the possibility of long coherence and interaction times of a few seconds, allowing multiple quantum gate operations.
Physical Review B | 2014
Sebastian Probst; A. Tkalcec; Hannes Rotzinger; D. Rieger; Jean-Michel Le Floch; Maxim Goryachev; Michael E. Tobar; Alexey V. Ustinov; Pavel Bushev
Low loss Bulk Acoustic Wave devices are considered from the point of view of the solid state approach as phonon-confining cavities. We demonstrate effective design of such acoustic cavities with phonon-trapping techniques exhibiting extremely high quality factors for trapped longitudinally-polarized phonons of various wavelengths. Quality factors of observed modes exceed 1 billion, with a maximum Q-factor of 8 billion and Q × f product of 1.6 · 1018 at liquid helium temperatures. Such high sensitivities allow analysis of intrinsic material losses in resonant phonon systems. Various mechanisms of phonon losses are discussed and estimated.
IEEE Transactions on Ultrasonics Ferroelectrics and Frequency Control | 2012
Maxim Goryachev; Serge Galliou; Philippe Abbé; Pierre-Yves Bourgeois; Serge Grop; Benoît Dubois
The confinement of high frequency phonons approaching 1 GHz is demonstrated in phonon-trapping acoustic cavities at cryogenic temperatures using a low-coupled network approach. The frequency range is extended by nearly an order of magnitude, with excitation at greater than the 200th overtone achieved for the first time. Such a high frequency operation reveals Rayleigh-type phonon scattering losses due to highly diluted lattice impurities and corresponding glasslike behavior, with a maximum Q(L)×f product of 8.6×10(17) at 3.8 K and 4×10(17) at 15 mK. This suggests a limit on the Q×f product due to unavoidable crystal disorder. Operation at 15 mK is high enough in frequency that the average phonon occupation number is less than unity, with a loaded quality factor above half a billion. This work represents significant progress towards the utilization of such acoustic cavities for hybrid quantum systems.