We demonstrate the strong coupling between an electron spin ensemble and a three-dimensional cavity in a reflection geometry. We also find that an anticrossing in the cavity/spin spectrum can be observed under conditions that the collective coupling strength is smaller than the spin linewidth or the cavity linewidth. We identify a ratio of to as a condition to observe a splitting in the cavity frequency. Finally, we confirm that scales with , where is the number of polarized spins.
REFERENCES
1.
D. F.
Walls
and G. J.
Milburn
, Quantum Optics
(Springer
, New York
, 2008
), Chap. 11.2.
M.
Brune
, F.
Schmidt-Kaler
, A.
Maali
, J.
Dreyer
, E.
Hagley
, J. M.
Raimond
, and S.
Haroche
, Phys. Rev. Lett.
76
, 1800
(1996
).3.
A.
Boca
, R.
Miller
, K. M.
Birnbaum
, A. D.
Boozer
, J.
McKeever
, and H. J.
Kimble
, Phys. Rev. Lett.
93
, 233603
(2004
).4.
A.
Wallraff
, D. I.
Schuster
, A.
Blais
, L.
Frunzio
, R. -S.
Huang
, J.
Majer
, S.
Kumar
, S. M.
Girvin
, and R. J.
Schoelkopf
, Nature (London)
431
, 162
(2004
).5.
F.
Brennecke
, T.
Donner
, S.
Ritter
, T.
Bourdel
, M.
Köhl
, and T.
Esslinger
, Nature (London)
450
, 268
(2007
).6.
Y.
Colombe
, T.
Steinmetz
, G.
Dubois
, F.
Linke
, D.
Hunger
, and J.
Reichel
, Nature (London)
450
, 272
(2007
).7.
P. F.
Herskind
, A.
Dantan
, J. P.
Marler
, M.
Albert
, and M.
Drewsen
, Nat. Phys.
5
, 494
(2009
).8.
J. M.
Fink
, R.
Bianchetti
, M.
Baur
, M.
Göppl
, L.
Steffen
, S.
Filipp
, P. J.
Leek
, A.
Blais
, and A.
Wallraff
, Phys. Rev. Lett.
103
, 083601
(2009
).9.
D. I.
Schuster
, A. P.
Sears
, E.
Ginossar
, L.
DiCarlo
, L.
Frunzio
, J. J. L.
Morton
, H.
Wu
, G. A. D.
Briggs
, B. B.
Buckley
, D. D.
Awschalom
, and R. J.
Schoelkopf
, Phys. Rev. Lett.
105
, 140501
(2010
).10.
Y.
Kubo
, F. R.
Ong
, P.
Bertet
, D.
Vion
, V.
Jacques
, D.
Zheng
, A.
Dréau
, J. -F.
Roch
, A.
Auffeves
, F.
Jelezko
, J.
Wrachtrup
, M. F.
Barthe
, P.
Bergonzo
, and D.
Esteve
, Phys. Rev. Lett.
105
, 140502
(2010
).11.
H.
Wu
, R. E.
George
, J. H.
Wesenberg
, K.
Mølmer
, D. I.
Schuster
, R. J.
Schoelkopf
, K. M.
Itoh
, A.
Ardavan
, J. J. L.
Morton
, and G. A. D.
Briggs
, Phys. Rev. Lett.
105
, 140503
(2010
).12.
H.
Paik
, D. I.
Schuster
, L. S.
Bishop
, G.
Kirchmair
, G.
Catelani
, A. P.
Sears
, B. R.
Johnson
, M. J.
Reagor
, L.
Frunzio
, L.
Glazman
, and R. J.
Schoelkopf
, arXiv:1105.4652 (unpublished).13.
P.
Imamoğlu
, Phys. Rev. Lett.
102
, 083602
(2009
).14.
J. H.
Wesenberg
, A.
Ardavan
, G. A. D.
Briggs
, J. J. L.
Morton
, R. J.
Schoelkopf
, D. I.
Schuster
, and K.
Mølmer
, Phys. Rev. Lett.
103
, 070502
(2009
).15.
I.
Chiorescu
, N.
Groll
, S.
Bertaina
, T.
Mori
, and S.
Miyashita
, Phys. Rev. B
82
, 024413
(2010
).16.
G.
Ilangovan
, J. L.
Zweier
, and P.
Kuppusamy
, J. Phys. Chem. B
104
, 4047
(2000
).17.
P.
Poole
, Jr., Electron Spin Resonance: A Comprehensive Treatise on Experimental Techniques
(Dover
, New York
, 1983
), Chap. 11.18.
In commercial EPR spectrometers, only the absorption signal is extracted while the dispersion signal is eliminated by the automatic frequency control circuitry, which locks the source frequency at the cavity dip position.
© 2011 American Institute of Physics.
2011
American Institute of Physics
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