We describe a method to map the standing-wave pattern inside an open-access Fabry–Perot optical cavity with sub-wavelength resolution by perturbing it with a commercially available tapered fiber. The method is applied to a fiber Fabry–Perot microcavity. We demonstrate its use in determining the relative position of the antinodes at two different wavelengths. In addition, we use the tapered optical fiber as a point-like source, allowing precise positioning of a microscope objective with respect to the cavity mode.
REFERENCES
1.
M. D.
Eisaman
, J.
Fan
, A.
Migdall
, and S. V.
Polyakov
, “Invited review article: Single-photon sources and detectors
,” Rev. Sci. Instrum.
82
, 071101
(2011
).2.
K.
Heshami
, D. G.
England
, P. C.
Humphreys
, P. J.
Bustard
, V. M.
Acosta
, J.
Nunn
, and B. J.
Sussman
, “Quantum memories: Emerging applications and recent advances
,” J. Mod. Opt.
63
, 2005
–2028
(2016
).3.
J.
Benedikter
, T.
Hümmer
, M.
Mader
, B.
Schlederer
, J.
Reichel
, T. W.
Hänsch
, and D.
Hunger
, “Transverse-mode coupling and diffraction loss in tunable Fabry–Pérot microcavities
,” New J. Phys.
17
, 053051
(2015
).4.
O.
Hosten
, N. J.
Engelsen
, R.
Krishnakumar
, and M. A.
Kasevich
, “Measurement noise 100 times lower than the quantum-projection limit using entangled atoms
,” Nature
529
, 505
–508
(2016
).5.
Z.
Zhiqiang
, C. H.
Lee
, R.
Kumar
, K. J.
Arnold
, S. J.
Masson
, A. S.
Parkins
, and M. D.
Barrett
, “Nonequilibrium phase transition in a spin-1 Dicke model
,” Optica
4
, 424
–429
(2017
).6.
E. J.
Davis
, G.
Bentsen
, L.
Homeier
, T.
Li
, and M. H.
Schleier-Smith
, “Photon-mediated spin-exchange dynamics of spin-1 atoms
,” Phys. Rev. Lett.
122
, 010405
(2019
).7.
S.
Garcia
, F.
Ferri
, K.
Ott
, J.
Reichel
, and R.
Long
, “Dual-wavelength fiber Fabry-Perot cavities with engineered birefringence
,” Opt. Express
26
, 22249
(2018
).8.
S.
Welte
, B.
Hacker
, S.
Daiss
, S.
Ritter
, and G.
Rempe
, “Cavity carving of atomic bell states
,” Phys. Rev. Lett.
118
, 210503
(2017
).9.
10.
J.
Gallego
, W.
Alt
, T.
Macha
, M.
Martinez-Dorantes
, D.
Pandey
, and D.
Meschede
, “Strong Purcell effect on a neutral atom trapped in an open fiber cavity
,” Phys. Rev. Lett.
121
, 173603
(2018
).11.
O.
Wiener
, “Stehende Lichtwellen und die Schwingungsrichtung polarisirten Lichtes
,” Ann. Phys.
276
, 203
–243
(1890
).12.
M.
Sasaki
, X.
Mi
, and K.
Hane
, “Standing wave detection and interferometer application using a photodiode thinner than optical wavelength
,” Appl. Phys. Lett.
75
, 2008
–2010
(1999
).13.
H.
Stiebig
, D.
Knipp
, and E.
Bunte
, “Standing-wave spectrometer
,” Appl. Phys. Lett.
88
, 083509
(2006
).14.
J. C.
Knight
, N.
Dubreuil
, V.
Sandoghdar
, J.
Hare
, V.
Lefèvre-Seguin
, J. M.
Raimond
, and S.
Haroche
, “Characterizing whispering-gallery modes in microspheres by direct observation of the optical standing-wave pattern in the near field
,” Opt. Lett.
21
, 698
(1996
).15.
S.
Gotzinger
, S.
Demmerer
, O.
Benson
, and V.
Sandoghdar
, “Mapping and manipulating whispering gallery modes of a microsphere resonator with a near-field probe
,” J. Microsc.
202
, 117
–121
(2001
).16.
A. F.
Koenderink
, M.
Kafesaki
, B. C.
Buchler
, and V.
Sandoghdar
, “Controlling the resonance of a photonic crystal microcavity by a near-field probe
,” Phys. Rev. Lett.
95
, 153904
(2005
).17.
N.
Rotenberg
and L.
Kuipers
, “Mapping nanoscale light fields
,” Nat. Photonics
8
, 919
–926
(2014
).18.
D.
Courjon
, C.
Bainier
, and F.
Baida
, “Seeing inside a Fabry-Pérot resonator by means of a scanning tunneling optical microscope
,” Opt. Commun.
110
, 7
–12
(1994
).19.
G. R.
Guthöhrlein
, M.
Keller
, K.
Hayasaka
, W.
Lange
, and H.
Walther
, “A single ion as a nanoscopic probe of an optical field
,” Nature
414
, 49
–51
(2001
).20.
I.
Favero
, S.
Stapfner
, D.
Hunger
, P.
Paulitschke
, J.
Reichel
, H.
Lorenz
, E. M.
Weig
, and K.
Karrai
, “Fluctuating nanomechanical system in a high finesse optical microcavity
,” Opt. Express
17
, 12813
(2009
).21.
A.
Gloppe
, P.
Verlot
, E.
Dupont-Ferrier
, A.
Siria
, P.
Poncharal
, G.
Bachelier
, P.
Vincent
, and O.
Arcizet
, “Bidimensional nano-optomechanics and topological backaction in a non-conservative radiation force field
,” Nat. Nanotechnol.
9
, 920
–926
(2014
).22.
F.
Fogliano
, B.
Besga
, A.
Reigue
, P.
Heringlake
, L. M.
de Lépinay
, C.
Vaneph
, J.
Reichel
, B.
Pigeau
, and O.
Arcizet
, “Cavity nano-optomechanics in the ultrastrong coupling regime with ultrasensitive force sensors
,” arXiv:1904.01140 [quant-ph] (2019
).23.
J. D.
Thompson
, B. M.
Zwickl
, A. M.
Jayich
, F.
Marquardt
, S. M.
Girvin
, and J. G. E.
Harris
, “Strong dispersive coupling of a high-finesse cavity to a micromechanical membrane
,” Nature
452
, 72
–75
(2008
).24.
A.
Vochezer
, T.
Kampschulte
, K.
Hammerer
, and P.
Treutlein
, “Light-mediated collective atomic motion in an optical lattice coupled to a membrane
,” Phys. Rev. Lett.
120
, 073602
(2018
).25.
D.
Hunger
, T.
Steinmetz
, Y.
Colombe
, C.
Deutsch
, T. W.
Hänsch
, and J.
Reichel
, “A fiber Fabry–Perot cavity with high finesse
,” New J. Phys.
12
, 065038
(2010
).26.
G.
Barontini
, L.
Hohmann
, F.
Haas
, J.
Esteve
, and J.
Reichel
, “Deterministic generation of multiparticle entanglement by quantum Zeno dynamics
,” Science
349
, 1317
–1321
(2015
).27.
R.
McConnell
, H.
Zhang
, J.
Hu
, S.
Ćuk
, and V.
Vuletić
, “Entanglement with negative Wigner function of almost 3,000 atoms heralded by one photon
,” Nature
519
, 439
–442
(2015
).28.
Y. R. P.
Sortais
, H.
Marion
, C.
Tuchendler
, A. M.
Lance
, M.
Lamare
, P.
Fournet
, C.
Armellin
, R.
Mercier
, G.
Messin
, A.
Browaeys
, and P.
Grangier
, “Diffraction-limited optics for single-atom manipulation
,” Phys. Rev. A
75
, 013406
(2007
).29.
C.
Robens
, S.
Brakhane
, W.
Alt
, F.
Kleißler
, D.
Meschede
, G.
Moon
, G.
Ramola
, and A.
Alberti
, “A high numerical aperture (NA = 0.92) objective lens for imaging and addressing of cold atoms
,” Opt. Lett.
42
, 1043
(2017
).© 2020 Author(s).
2020
Author(s)
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