We show that when a microsphere is illuminated by an evanescent wave, the optical forces on- and off-whispering gallery mode (WGM) resonance can differ by several orders of magnitude. Such size-selective force allows one to selectively manipulate the resonating particles, while leaving those particles at off-resonance untouched. As WGM resonances have very high-Q’s, this kind of force could be deployed for size-selective manipulation with a very high accuracy (1Q), as well as simultaneous particle-sorting according to their size or resonant frequency.

1.
P. T.
Korda
,
M. B.
Taylor
, and
D. G.
Grier
,
Phys. Rev. Lett.
89
,
128301
(
2002
).
2.
M. P.
Macdonald
,
G. C.
Spalding
, and
K.
Dholakia
,
Nature (London)
426
,
421
(
2003
).
3.
M.
Righini
,
A. S.
Zelenina
,
C.
Girard
, and
R.
Quidant
,
Nat. Phys.
3
,
477
(
2007
).
5.
A.
Fontes
,
A. A. R.
Neves
,
W. L.
Moreira
,
A. A.
de Thomaz
,
L. C.
Barbosa
,
C. L.
Cesar
, and
A. M.
de Paula
,
Appl. Phys. Lett.
87
,
221109
(
2005
).
6.
T.
Carmon
,
H.
Rokhsari
,
L.
Yang
,
T. J.
Kippenberg
, and
K. J.
Vahala
,
Phys. Rev. Lett.
94
,
223902
(
2005
).
7.
M.
Eichenfield
,
C. P.
Micheal
,
R.
Perahia
, and
O.
Painter
,
Nat. Photonics
1
,
416
(
2007
).
8.
P.
Chylek
,
J. T.
Kiehl
, and
M. K. W.
Ko
,
Phys. Rev. A
18
,
2229
(
1978
).
9.
We note that the theoretical work in Ref. 8 used plane incident wave, whereas the experimental works in Refs. 4 and 5 used focused beams. For focused beams, the enhancement in the optical force will depend a lot on the position of the beam’s focus with respect to the sphere (see Ref. 5).
10.
T.
Mukaiyama
,
K.
Takeda
,
H.
Miyazaki
,
Y.
Jimba
, and
M.
Kuwata-Gonokami
,
Phys. Rev. Lett.
82
,
4623
(
1999
).
11.
Optical Microcavities
, edited by
K. J.
Vahala
(
World Scientific
,
Singapore
,
2004
), Chap. 5.
12.
Y.
Hara
,
T.
Mukaiyama
,
K.
Takeda
, and
M.
Kuwata-Gonokami
,
Opt. Lett.
28
,
2437
(
2003
).
13.
P.
Chylek
,
V.
Ramaswamy
,
A.
Ashkin
, and
J. M.
Dziedzic
,
Appl. Opt.
22
,
2302
(
1983
).
14.
Y. P.
Rakovich
,
J. F.
Donegan
,
M.
Gerlach
,
A. L.
Bradley
,
T. M.
Connolly
,
J. J.
Boland
,
N.
Gaponik
, and
A.
Rogach
,
Phys. Rev. A
70
,
051801
(
2004
).
15.
J.
Ng
,
C. T.
Chan
,
P.
Sheng
, and
Z. F.
Lin
,
Opt. Lett.
30
,
1956
(
2005
).
16.
M. L.
Povinelli
,
S. G.
Johnson
,
M.
Loncar
,
M.
Ibanescu
,
E. J.
Smythe
,
F.
Capasso
, and
J. D.
Joannopoulos
,
Opt. Express
13
,
8286
(
2005
).
17.
S.
Kawata
and
T.
Sugiura
,
Opt. Lett.
17
,
772
(
1992
).
18.
Resonant optical force induced by an evanescent wave was considered by Chang in the Mie regime. We remark that unlike the WGM regime consider here, the Mie regime lacks size selectivity. See, e.g.,
S.
Chang
,
J. T.
Kim
,
J. H.
Jo
, and
S. S.
Lee
,
Opt. Commun.
139
,
252
(
1997
).
19.
M.
Lester
and
M.
Nieto-Vesperinas
,
Opt. Lett.
24
,
936
(
1999
).
20.
M.
Gu
,
J.-B.
Haumonte
,
Y.
Micheau
,
J. W. M.
Chon
, and
X.
Gan
,
Appl. Phys. Lett.
84
,
4236
(
2004
).
21.
K.
Grujic
and
O. G.
Helleso
,
Opt. Express
15
,
6470
(
2007
).
22.

The fact that Eq. (1) is a function of rs is merely a consequence of choosing different coordinate origins for particles with different sizes, i.e., the origin is rs+λ2 from the interface where the intensity is fixed.

23.
P. J.
Reece
,
V.
Garces-Chavez
, and
K.
Dholakia
,
Appl. Phys. Lett.
88
,
221116
(
2006
).
24.
V.
Garces-Chavez
,
R.
Quidant
,
P. J.
Reece
,
G.
Badenes
,
L.
Torner
, and
K.
Dholakia
,
Phys. Rev. B
73
,
085417
(
2006
).
25.
G.
Volpe
,
R.
Quidant
,
G.
Badenes
, and
D.
Petrov
,
Phys. Rev. Lett.
96
,
238101
(
2006
).
26.
J.
Ng
,
Z. F.
Lin
,
C. T.
Chan
, and
P.
Sheng
,
Phys. Rev. B
72
,
085130
(
2005
).
27.

The optical force is a quadratic function of the fields. At resonance, the WGM’s field is dominating over the incident field. The force induced solely by the incident field is negligibly small, whereas the force induced solely by the WGM’s field is identically zero owing to symmetry. As a result, FWGM is a bilinear product of the incident driving field and the WGM’s field.

You do not currently have access to this content.