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Whispering-Gallery Mode Microlasers
— from microdisk resonator to square resonator
Huang Yong-Zhen (黄永箴) Institute of Semiconductor, State Key Lab on Integrated
Optoelectronics Chinese Academy of Sciences
报告提纲
I. 光学微腔及应用
II. 直连波导的微盘激光器
III. 正方形微腔激光器
IV. 集成的微腔激光器
2
Fabry-Pérot cavity:vertical-cavity surface-emitting lasers
• Whispering-Gallery mode microcavity: microdisk laser
• Photonic Crystal microcavity
K. J. Vahala, Nature vol.424, p. 839 (2003)
Microcavities
3
VCSEL-有源光缆光互连应用
(a)2003年 服务器电缆;(b)2000年HP电缆;(c)
标准PCIe-x16电缆; (d)2007年有源光缆. 电缆传输距离2~3m,光缆传输距离100m 4
直调光子晶体激光器~fJ/bit数据传输
Nature Photon., vol. 7, p.569(2013) 5
Opt. Exp., vol.17, p.11107(2009) “Thresholdless nanoscale coaxial lasers”
Nature, vol. 482, p.204, 2012.
等离子激元纳激光器(金属层限制)
Nature mater., vol. 10, p. 110( 2011)
6
Nature Commun. DOI:10.1038/ncomms3822(2013)
Electrically driven nanobeam lasers
7
Whispering-Gallery Mode
L. Rayleigh,The problem of the whispering
gallery, Phil. Mag., 20, 1001(1910)
Echo-wall of Heaven Temple
Heaven Temple
St. Paul’s Cathedral
8
Total internal reflection
S. L. McCall et al, Appl. Phys. Lett., vol.60, 289 (1992), Electron. Lett.,
vol.28, p.1010(1992), Appl. Phys. Lett., vol.83, p.797(2003)
Optical microdisk lasers
a) Geometrical optics and b) wave optics
representation of a whispering gallery mode Adv. Matt., vol.25, p.707(2013)
9
Directional emission microdisk lasers
(d) Science, 280, 1556(1998); (e) Appl. Phys. Lett., 83, 710(2003), (f) IEEE Photon. Technol. Lett., 15,1330(2003)
Nature Photon., vol.4, p.182(2010) PNAS, 107, 22407(2010)
10
Droplet microlaser
Laser Photon Rev.,vol.7, p.60(2013)
11
L. Ge, et al, “Rotation-induced evolution of far-field emission
patterns of deformed microdisk cavities”, Optica, vol.2, p.323
(2015)
Rotation related far-field emission patterns 片上光学陀螺
10-13 ~6 rad/s 12
Microresonator frequency comb
Microresonator frequency comb optical
clock, Optica, vol.1, p.10(2014)
13
Light-trapping diamond waveguide for sensing
“Broadband magnetometry and
temperature sensing with a light-
trapping diamond waveguide”,
Nature Phys DOI:
10.1038/NPHYS3291(2015)
氮空位
14
PNAS,vol.111,p.E3836(2014)
Raman microlaser for detecting nanoparticles
15
Whispering-gallery microlaser in living cells
Nano.Lett.,15, 5647-5652(2015)
折射率1.60:1.375
半径5~10微米
NATURE PHOTONICS DOI:
10.1038/NPHOTON.2015.129
(2015)
16
报告提纲
I. 光学微腔及应用
II. 直连波导的微盘激光器
III. 正方形微腔激光器
IV. 集成的微腔激光器
17
Mode solution for 2D microdisk resonators
Mode field distribution in a 2D microdisk with a radius of R:
0
(1)00(1)
0
( , ) ( )exp( )
( )( , ) ( )exp( )
( )
z v
vz v
v
F r AJ nk r iv r R
J nk RF r A H k r iv r R
H k R
(1)' ' (1)
0 0 0 0( ) ( ) ( ) ( )v v v vJ nk R H k R J nk R H k R
Eigenvalue equation for calculating mode wavelengths and mode Q
factors:
Jv(x) and Hv(1)(x) are Bessel function and first kind Hankel function, for
TM and TE modes η = n and 1/n, respectively.
M. Hentschel et al, Phys. Rev. E 66, 056207 (2002). 18
WG mode field patterns in a circular resonator with a
diameter of 4.5 μm and refractive index of 3.2.
Superposition of TM18,3 and
TM15,4 with phase difference
of (a) π and (b) 0.
Analytical solution.
TM18,1 TM18,2 TM18,3 TM15,4
±
19
1540 1545 1550 1555 156010-5
10-4
10-3
10-2
10-1
100
Q = 6.7x104
Inte
nsity (
a.u
.)
Wavelength (nm)
Three ports
Four ports
5.36x103
Opt. Exp., vol.17, p.23010(2009), Semi. Sci. Techonol., vol.25, 105005(2010)
Mode coupling and directional emission for microdisk
1.40 1.45 1.50 1.55 1.6010
-6
10-5
10-4
10-3
10-2
10-1
100
101
1.49 1.4902 1.490410
-3
10-2
10-1
100
Inte
nsity (
a.u
.)
Wavelength (m)
(a)perfect microdisk
1.40 1.45 1.50 1.55 1.6010
-6
10-5
10-4
10-3
10-2
10-1
100
Inte
nsi
ty (
a.u
.)
Wavelength (m)
Symmetric
Antisymmetric
(b)
d
nO
R
Diameter 4.5μm microdisk connected a 0.6μm output waveguide
Radius 10μm microdisk connected three and four 2μm output waveguides
20
1530 1540 1550 1560 1570
-60
-50
-40
-30
-20
-10
45mA, 290K
Inte
nsi
ty (
dB
)
Wavelength (nm)
Rin= 0(a)
28.4dB
2.29nm
11.08nm
Unidirectional microdisk and microring laser
(radius 10 m)
J. Opt. Soc. Am. B, vol. 31, p.2773(2014) 21
22
2 4 6 8 10 12 14 16 18 20-15
-12
-9
-6
-3
0
3
6
9
Modulation Frequency (GHz)
Modula
tion R
esponse
(dB
)
12 mA
15 mA
18 mA
15.2 GHz
2 4 6 8 10 12 14 16 18 20-15
-12
-9
-6
-3
0
3
6
9
Modula
tion R
esponse
(dB
)
Modulation Frequency (GHz)
10 mA
15 mA
20 mA
13.0 GHz
Microring laser Microdisk laser
R = 15 μm, d = 7 μm, W = 2 μm R = 15 μm, W = 2 μm
(a)
Influence of carrier spatial hole burning and
diffusion on high speed modulation
Appl. Phys. Lett., vol. 104, 161101(2014)
Mode field pattern
23
Size limit for microdisk lasers with vertical semiconductor
waveguide-vertical radiation loss
1380 1400 1420 1440 1460 1480 1500-80
-60
-40
-80
-60
-40
-80
-60
-40
1380 1400 1420 1440 1460 1480 1500
0.62 nm
(c)
Wavelength (m)
R = 3.25 m
I = 3 mA
0.25 nm
(b) R = 3.5 m
I = 1.5 mA
Inte
nsity (
dB
m)
0.2 nm0.056 nm
R = 3.75 m
I = 1 mA
(a)3.0 3.5 4.0 4.5 5.0 5.5
0.0
0.5
1.0
1.5
2.0
Radius (m)
Th
resh
old
Cu
rre
nt
(mA
)
0
2
4
6
Thre
shold
Curr
ent D
ensity (
kA
/cm
2)
T = 288 K
1380 1400 1420 1440 1460 1480 150010
2
103
104
105
Mode B
Q
Wavelength (nm)
R = 3 m
R = 3.25 m
R = 3.5 m
R = 3.75 m
Mode A
Mode Q factors obtained by 3D FDTD
Threshold current versus disk radius
J. Opt. Soc. Am. B, vol.32, p.439(2015)
报告提纲
I. 光学微腔及应用
II. 直连波导的微盘激光器
III. 正方形微腔激光器
IV. 集成的微腔激光器
24
Triangle Square Octagon
Different whispering-gallery mode microlasers
IEEE J. Sel. Top. Quantum
Electron., vol.19, 1501808 (2013) IEEE Photon Technol
Lett, vol. 19, p. 963(2007)
Opt. Lett., vol.33, p.2170
(2008) IEEE Photon. J., vol.3,
p.756(2011) 25
Our SCI papers about square and microdisk resonators
JQE: IEEE J. Quantum Electron.; PTL: IEEE Photon. Technol. Lett.; OL: Opt. Lett.; APL: Appl. Phys. Lett.
COL: Chin. Opt. Lett.; JLT: J. Lightwave Technol.; OE: Opt. Exp.; EL: Electron. Lett., JAP: J. Appl. Phys. 26
2002 2004 2006 2008 2010 2012 2014 20160
2
4
6
8
10
SC
I P
ap
er
Nu
mb
ers
Year
JQE2
PTL+OL+COL+JQE
APL+JQE+PTL2+EL+JAP+JOSAB
JSTQE+El2+QE2+OE2
+APL+PJ+JOSAB+OEng
JLT+OL+PTL+OE
+SCI China
Square resonator
microdisk+microring
2D rectangular microresonator
reduced to three-layer slab waveguides in x and y-directions
W5
W4
W3
W2
W1
z
C4
-1 C4
C2
x
ys
y
sd
''
sd
'
sx
W. H. Guo, et al, IEEE J. Quantum Electron., vol. 39, p.1563 (2003)
Y. D. Yang, et al, IEEE J. Quantum Electron., vol. 43, p.497(2007)
Fz (p, q) = Fzxp(x) Fzyq(y)
2
0
2
1
22 )1( kn 2
0
2
1
22 knyx
cos( ) / 2
cos( / 2 )exp[ ( / 2)] / 2
cos( / 2 )exp[ ( / 2)] / 2
x x
p
zx x x x
x x x
x x a
F a x a x a
a x a x a
cos( ) / 2
cos( / 2 )exp[ ( / 2)] / 2
cos( / 2 )exp[ ( / 2)] / 2
y y
q
zy y y y
y y y
y y b
F b y b y b
b y b y b
tan( / 2 )
tan( / 2 )
x x x x
y y y y
a
b
For TE mode = n1
2/n22
For TM mode = 1, v = x, y
27
Y. D. Yang, et al., IEEE J. Quantum. Electron., 43, 497, 2007.
2.0 2.1 2.2 2.3 2.4175
180
185
190
195
200
205
102
103
104
Qu
alit
y fa
cto
r
Fre
qu
en
cy (
TH
z)
Length a (m)
Mode A
Mode B
175 180 185 190 195 200 20510
-4
10-3
10-2
10-1
100
101
Mode B
No
rma
lize
d in
ten
sity
Frequency (THz)
a = 2 m
2.16 m
2.4 m
Mode A
High Q mode has field distribution anti-symmetry to the diagonals of resonator
High Q mode with small vertex radiation loss
Field patterns of electric field component
Ez obtained by FDTD simulation for the
mode A with the length of (a, d) 2 m,
(b,e) 2.16 m, and (c,f) 2.4 m.
Mode A
Mode B
28
Analytical electric filed patterns for (a) TM6,8, (b) TM5,9, and (c) TM4,10 in square
resonator with side length 2.5 µm and refractive index 3.2
Electric field patterns for (a) TM6,8and(b) TM4,8 in square
resonator with side length 2.5 µm and a output waveguide
Mode field pattern for square resonators
Light ray analysis IEEEJ.Quantum Electron. vol.39,
p.1106(2003), vol.46,p.414(2010)
29
InP
AlGaInAs QWs
SiO2
SiNx
BCB
P-electrode
N-electrode
Etching BCB Opening p-electrode
window
Forming
electrodes
Planized by filling BCB Photolithography and
ICP etching
Fabrication technique process
30
Square microlasers with different output waveguides
0 10 20 30 40 500
100
200
300
400
500
y
x
z
PMMF
PSMF×3
Voltage
I (mA)
Po
wer
(μ
W)
0.0
0.3
0.6
0.9
1.2
1.5
1.8V
olt
age
(V)
(a)
1520 1530 1540 1550 1560 1570 1580 1590
-70
-60
-50
-40
-30
-20
-10
40
32
24
16
8
B
Wavelength (nm)
Inte
nsi
ty (
dB
m)
Cur
rent
( m
A)
(a) A
Powers coupled into MMF and SMF versus CW current, and lasing spectra at 8, 16, 24, 32
and 40 mA for microlaser with side length 16m and 2m wide vertex output waveguide.
Sci China-Phys Mech Astron vol. 58, 114205(2015)
1520 1530 1540 1550 1560 1570 1580
-70
-60
-50
-40
-30
-20
-10
Inte
nsi
ty (
dB
m)
Wavelength (nm)
24 mA
SMSR:41 dB
91
92
93
94
95
96
97
98
99
100
p+
q
IEEE J. Quantum Electron., vol. 50, p.981(2014)
2 2
, 2 / [( 2) / ] [( 2) / ]p q x yan p q
31
1.0 1.2 1.4 1.6 1.8 2.0
8.0x104
1.6x105
2.4x105
3.2x105
4.0x105
Width of output waveguide (μm)
Mo
de Q
facto
r
TEo,(52,56)
TEo,(51,55)
TEo,(50,54)
TEo,(49,53)
(b)
1.0 1.2 1.4 1.6 1.8 2.0
2.0x104
4.0x104
6.0x104
8.0x104
TEo,(52,56)
TEo,(51,55)
TEo,(50,54)
TEo,(49,53)
Width of output waveguide (μm)
Mo
de Q
facto
r
(a)
Mode Q factors versus the output waveguide width
at (a) g = 0 and (b) g = 2 cm-1 in square resonator
with the side length of 17.8 m. a = 17.8 m and w = 1.8 m
Single mode square microlaser
32
Square microlaser with the side length
of 17.8 m and the output waveguide
width of 1.4 m
Based on the redshift rate, the
temperature rise of 81 K is obtained from
5 to 65 mA and the practical laser
temperature is about 379 K at 65 mA.
Opt. Exp., vol. 23, p.27739(2015)
Single mode square microlaser
33
Transverse mode wavelength interval modulated by refractive index distribution
10 15 20 25 30
0.3
0.6
0.9
1.2
1.5
1.8
Δλ
(nm
)
a (μm)
-10 -5 0 5 10
-10
-5
0
5
10
-1
-0.5
0
0.5
1
(a)
-10 -5 0 5 10
-10
-5
0
5
10
-1
-0.5
0
0.5
1
(b)
Mode wavelength intervals versus Δn for square resonators with a = 20 μm, wg =
1.5 μm, W = 2 μm, and a = 30 μm, wg = 2.5 μm, W = 4 μm.
-5 -4 -3 -2 -1 0 1 2 3 4 50.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4 a = 20 m, W = 2 m
a = 30 m, W = 4 m
(nm
)
n (×10-3)
34
35
0 20 40 60 80 1000
100
200
300
400
500
PMMF
PSMF
× 4
Po
wer
(μ
W)
Current (mA)
0.0
0.3
0.6
0.9
1.2
1.5
1.8
Vo
ltag
e (V
)
1540 1545 1550 1555 1560 1565 1570 1575 1580 1585
-70
-60
-50
-40
-30
-20
Inte
nsi
ty (
dB
)
Wavelength (nm)
90 mA
85 90 95 100 105 110 115
0.24
0.28
0.32
0.36
0.40
Δλ
(nm
)
Current (mA)
-30
-20
-10
0
10
20
30
Intensity ratio
Inte
nsi
ty r
atio
(d
B)
current: 89 ~ 109 mA
Δλ: 0.25 ~ 0.39 nm
Δf: 30 ~ 48 GHz
注入窗口
FWM
a = 30 μm, w = 2.5 μm, current injection
region width W = 4 μm
Lasing characteristics of dual transverse modes
36
EDFA OBPFPD
ESA
DC bias
Schematic diagram for microwave generation based on the dual-mode microsquare laser
Microwave frequency of 30.56、32.70、35.12、39.51 GHz at current of 90, 95, 100, and 105 mA.
Opt. Lett. Vol. 40, p.3548(2015)
Tunable microwave based on the dual mode laser
1561 1562 1563 1564 1565 1566
-60
-30
0
30
60
90
120
105 mA
100 mA
95 mA
Inte
nsi
ty (
dB
)
Wavelength (nm)
90 mA
27 30 33 36 39 42-70
-65
-60
-55
-50
-45
-40
-35
-30
-25
105 mA100 mA95 mA90 mA
Inte
nsi
ty (
dB
)
Frequency (GHz)
a = 16 m ,w = 1.5 m, δ = 0, 0.5, 0.9, 1.3 μm
Deformed Sqaure resonator with high Q factor and enhanced transverse mode interval
37
THz wave generation based on deformed square microlasers
Corresponding to 0.43,
0.31and 0.16 THz
38
a = 16 m ,w = 1.5 m, δ = 0, 0.5, 0.9, 1.3 μm
报告提纲
I. 光学微腔及应用
II. 直连波导的微盘激光器
III. 正方形微腔激光器
IV. 集成的微腔激光器
39
40
互注入双圆微腔激光器
a) ICP刻蚀后的
SEM照片 b) 器件的显微镜
照片
a) PI曲线 b) 光谱
自由工作状态 激光器A和B:
Appl. Phys. Lett. vol.106, 191107(2015)
41
Ia=29 mA
互注入双圆微腔激光器
Ib=20 mA
42
张弛振荡峰高度:4.8 dB
张弛振荡频率:9.6 GHz
3dB带宽:14.65 GHz
张弛振荡峰高度:3.8 dB
3dB带宽:16.6 GHz
张弛振荡峰高度:1.4 dB
3dB带宽:16.0 GHz
互注入双圆微腔激光器
0 20 40 60 800.0
0.5
1.0
1.5
2.0
2.5
3.0
L-I
L-I
Outp
ut pow
er
(mW
)
FP injection current (mA)
ISQ = 0
ISQ = 10 mA
SMF
287 K
V-I
0.5
1.0
1.5
2.0
Voltage(V
)
单模光纤耦合输出功率2.8 mW
正方形边长a = 15 μm;
FP腔宽度 d = 2 μm 长度 L= 300 μm
1520 1530 1540 1550 1560 1570
-70
-60
-50
-40
-30
fp: 1 mA
squ: 10 mA
Inte
nsity (
dB
m)
Wavelength (nm)
14.9 nm
-60
-40
-20
0
fp: 40 mA
squ: 10 mASMSR: 50 dB
SMSR: 27 dB
WG-FP耦合模:SMSR = 50 dB
正方形WG模:SMSR = 27 dB
FSR = 14.9 nm
高速单模定向输出WG-FP耦合微腔激光器
43
0
30
60
90
120
150
180
CC laser
In-plane远场发散角~30°
小信号直接电流调制FP腔:
光谱随FP腔注入电流变化(ISQ = 10 mA) 稳定单模工作,不跳模
光谱随square腔注入电流变化(IFP = 40 mA)
0 3 6 9 12 15 18-12
-6
0
6
13 GHzM
od
ula
tio
n R
esp
on
se
(d
B)
Modulation Frequency (GHz)
FP:25 mA
FP:40 mA
FP:55 mA
ISQ = 10 mA
13 GHz
高速单模定向输出WG-FP耦合微腔激光器
44
图3光谱图与FP腔电流关系,10~70mA单模激射没跳模,对应激射模波长红移3.3nm。由此推断温度上升33K。
0 20 40 60 80
0
1
2
3
4
5
Po
we
r (m
W)
Current(mA)
290K
287K
ISQ
= 10 mA
-60
-40
-20
0
1520 1525 1530 1535 1540 1545 1550 1555 1560 1565 1570 1575 1580
-70
-60
-50
-40
-30
Inte
nsity (
dB
m)
FP:50 mA
square:10 mA
(a)
FP:5 mA
square:10 mA
Inte
nsity (
dB
m)
Wavelength (nm)
(b)
图1. 单模光纤耦合功率与FP腔电流关系,正方形腔电流10
图2. 激光光谱正方形腔和FP腔电流(a)10mA和50mA,边模抑制比48dB;(b) 5mA和10mA.
另一激光器结果:
45
46