exciton-polaritons in van der waals heterostructures in...
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Exciton-polaritons in van der Waals heterostructures in tunable microcavities
Alexander Tartakovskii Department of Physics and Astronomy
University of Sheffield, UK
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Inorganic Semiconductors Group in Sheffield http://ldsd.group.shef.ac.uk
Microcavity polaritons, quantum dot physics, III-V photonics (photonic crystals, waveguides), III-V device technology including crystal growth
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Light emitters in 2D heterostructures coupled to photonic devices
Polariton physics
TMDC/graphene LEDs
2D PHOTONICS
Photonic crystal nano-cavities
Tunable microcavities
2D
het
ero
stru
ctu
res
Schwarz Nano Lett (2014)
Withers Nat Materials (2015)
Dufferwiel, submitted
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Contributions
‘Open access cavity’ experiments with 2D materials in Sheffield: S Dufferwiel, S Schwarz, F Li, P Walker, M Sich, D Krizhanovskii, M Skolnick
2D materials and LED optics experiments in Sheffield: O Del Pozo Zamudio, R Schofield, O Skrypka, T Godde
2D heterostructures: F Withers & K Novoselov (Manchester)
Concave mirror design & fabrication: A Trichet & J Smith (Oxford)
Dielectric layer deposition: C Clark (Helia Photonics)
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Microcavities
- Strong vs weak coupling regimes
- Open tunable microcavities
MoSe2/hBN heterostructures
- Single and double ‘QWs’
Strong light-matter coupling in MoSe2/hBN QWs
- Neutral vs charged exciton-polaritons
Monolithic microcavity LEDs
- WSe2/hBN/graphene LED heterostructures
Talk outline
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Light emitters in optical cavities: ‘weak coupling’
600 700 800 9000.0
0.2
0.4
0.6
0.8
1.0
stop-band
Re
fle
ctivity
Wavelength (nm)
cavity
mode
Modification of emission spectrum and directionality
V
Q
nFP
3
24
3
Purcell enhancement of spontaneous emission rate dependent on the cavity quality factor (Q) and mode volume (V)
Weak coupling regime: Cavity and emitter dissipation rates exceed cavity-emitter coupling rate
Role of optical cavities: Control of light emission properties and light-matter interaction
Example of III-V planar microcavity
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Wu et al, Nature (2015)
Lasing in WSe2 films coupled to a photonic crystal nano-cavity
660 670 680 690 700 710
0
50
100
150
200
250
300
600 610 620 630
0
200
400
600
800
1000
half-cavity
full cavity with Rc
5.6m, x0.05
10m, x0.1
16m, x0.2
Ph
oto
lum
ine
sce
nce
in
ten
sity (
co
un
ts/s
/sq
.mic
ron
)
Wavelength (nm)
(a) half-cavity
full cavity:
Rc=25m
(b)
Schwarz et al, Nano Lett. (2014)
2D materials in the weak coupling regime
Purcell enhancement for GaSe and MoS2 in tunable cavities
WSe2 LEDs in monolithic microcavities: electroluminescence into cavity modes
1.50 1.55 1.60 1.65 1.70 1.750.0
0.2
0.4
0.6
0.8
1.0 no top mirror
full cavity
No
rma
lised
ele
ctr
olu
min
escen
ce in
ten
sity
Photon energy (eV)
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Strong coupling regime
Cavity-emitter coupling rate exceeds the cavity and emitter dissipation rates
-5 0 5-5
0
5
-5 0 50.0
0.5
1.0
EX
Ec
LPB
En
erg
y (
meV
)Detuning (meV)
Wrabi
UPB
(b)
|X|2
Detuning (meV)
|C|2
(a)
Composite bosons which inherit nonlinear component from excitons and allow direct access to polarisation and dispersion via out-coupling through cavity mirrors
224 phXRabi g
Formation of part-light-part-matter exciton-polaritons
LPB
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Exciton-polaritons in planar microcavities
Previous work: GaAs, organic microcavities with J-aggregates, GaN, CdTe, ZnO
Exciton
Photon
Upper Polariton
Lower polariton
Polariton condensate, superfluidity, polariton laser
Kasprzak Nature (2006)
k||
E
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TMDCs: properties relevant for polariton physics
- Transition from indirect to direct band-gap semiconductor
- Very large exciton binding energy (100s of meV)
- Very large oscillator strength (~40 times larger than in GaAs)
Kin Fai Mak et al, PRL (2010) Chernikov et al, PRL (2014)
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Z
Y
X
Z
Y
X
Tilt
Tilt
Z
XY
TopPiezoNanoposi oners
Bo omPiezoNanoposi oners
Bo omDBRmirror/sample
0.55NAAsphericLens
Adjustableheightlenstube
TopDBRmirror
Titaniumsampleholder
Titaniumsampleholder
Bottom XYZ stage and tilt-stages
Top XYZ stage
Bottom DBR
Free space optical access
Sample holder
Top mirror
Objective lens
- Microcavity formed by two independent dielectric distributed Bragg reflectors (DBRs)
-Top mirror - array of concave DBRs
- Spatial and spectral tuning at low and room temperature
‘Open access’ cavity system
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Optical mode
SiO2/TiO2 DBR
2D sample
- 2D film (or 2D heterostructure) placed on the flat DBR
- Any spot on 2D film can be selectively excited
- Size of the cavity mode on the bottom DBR ~1
- Mode tuned spectrally by adjusting the cavity length
Schwarz et al Nano Letters (2014) Dufferwiel et al APL (2014) Besga et al arXiv:1312.0819 Greuter al arXiv:1408.1357
2D layers in open microcavities
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Double and single ‘quantum well’ structure
Double QW region
Single QW region
Samples made by F. Withers
hBN
MoSe2
hBN
MoSe2
hBN
MoSe2
Single QW
Rabi splitting is expected to increase for multiple QWs:
QWRabi N
Double QW
Structure placed at the bottom planar DBR at an E-field antinode
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Typical PL spectrum consists of neutral and charged exciton peaks with narrow linewidths of 11 meV and 15meV
X0
X-
Photoluminescence of MoSe2 heterostructures
1.55 1.60 1.65 1.700
50000
100000
150000
200000
250000
300000
X0
7.5 meV
PL In
ten
sity (
cts
/sec)
Photon energy (eV)
T=6K, PL
4 QW device
X-
16.2 meV
4 QW device surprisingly shows even narrower PL peaks with linewidth of 7.5 meV for X0
Ross, Nat Comms (2013), Li PRL (2014)
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LPB
UPB
-Clear anticrossing observed in PL between cavity mode resonances and neutral exciton
-Spectrum at resonance shows well resolved polariton eigenstates
-Rabi splitting is 20 meV corresponding to exciton life-time of 0.4 ps (linewidth 1.6 meV)
Anticrossing
Strong exciton-photon coupling in a single QW
See also Liu et al, Nat Photonics (2015)
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Linewidth broadening when in resonance with X-
Intermediate coupling with X-: polariton modes unresolved
Splitting of ~9 meV observed for X- in reflectivity
Single QW region
X-
Broadening Anticrossing
LPB UPB
‘Intermediate’ coupling regime for X-
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Anticrossing shows an increased Rabi splitting of 29 meV in the double QW Consistent with the expected scaling with QW number:
Key stepping stone to observe room temperature strong coupling
Strong coupling for double-QW
QWRabi N
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Glass substrate Glass substrate
Bottom DBR
SiO2/NbO2 DBR
Glass substrate
Bottom DBR
Glass substrate
Bottom DBR
Top DBR 2D
structure DBR
Fabrication of monolithic microcavities
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Electroluminescence device (‘EL device’) Graphene h-BN WSe2 h-BN Graphene h-BN
-Single monolayer WSe2 flakes
-BN-WSe2-BN ‘sandwiches’
-WSe2 ‘EL devices’
Samples by Freddie Withers (Manchester)
EL device on DBR
DBR
WSe2 LED heterostructure in microcavity
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1.50 1.55 1.60 1.65 1.70 1.750.0
0.2
0.4
0.6
0.8
1.0 no top mirror
full cavity
N
orm
alis
ed
ele
ctr
olu
min
esce
nce
in
ten
sity
Photon energy (eV)
LEDs in monolithic microcavities
EL T=200 K
Strong electroluminescence coupled in the cavity mode(s)
1.56 1.60 1.64 1.680
200
400
600
0o
3o
6o
9o
12o
15o
18o
1.5 1.6 1.70.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
Ele
ctr
olu
min
escence inte
nsity (
cts
/s)
21o
PL
PL
EL
EL
full
cavity, 0o
full
cavity, 0o
no top
DBR
no top
DBR
Norm
aliz
ed P
L/E
L inte
nsity
Photon energy (eV)
T=300 K
Complex mode structure of ‘photonic dots’ formed due to finite thickness of the LED device
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Summary
http://ldsd.group.shef.ac.uk/research/2d-materials/
- Versatile microcavity technology for 2D materials research and applications demonstrated
Papers: Sercombe et al, Scientific Reports (2013); Schwarz et al, Nano Letters (2014); Del Pozo Zamudio et al, arxiv (2015); Withers et al, Nature Materials (2015)
-Strong exciton-photon coupling leading to formation of exciton-polaritons
- First electrically pumped 2D microcavity devices: prototype for vertically emitting lasers