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Time-resolved сathodoluminescence
What is time-resolved cathodoluminescence?
• Time-resolved cathodoluminescence is a technique in which
the time dynamics of the cathodoluminescence emission
process is observed
• Main imaging techniques:
1. Lifetime imaging
2. g(2) imaging
How does cathodoluminescence work?
When a sample is bombarded by fast electrons,
the material becomes excited as it returns to a
grounded state, it emits light.
The radiation that is generated in the
ultraviolet/visible/near-infrared regime of the
electromagnetic spectrum is referred to as
cathodoluminescence (CL) as the radiation is
generated by cathode rays (fast electrons).
This data can be collected with nanoscale
resolution and can reveal contrasts that cannot
be observed with any optical microscopy
technique.
Lifetime cathodoluminescence imaging
• Lifetime (or decay trace) mapping is one of the time-resolved techniques
• The method can be used to obtain insight into a large variety of physical
processes and material properties
• To perform lifetime cathodoluminescence imaging, a pulsed electron
microscope is required
Lifetime Imaging Mod
e
Spontaneous light emission process in time
Lifetime Imaging Mod
e
To study lifetime imaging,
a fast photodetector such
as an avalanche
photodiode (APD) or
photomultiplier tube (PMT)
can be used to detect
single photons with high
sensitivity and timing-
precision
Detection
Lifetime Imaging Mod
e
Application of lifetime imaging technique
CL decay-trace measurements can be used for a large range of applications
The extracted lifetime measurements are valuable to obtain information on
intrinsic material properties as well as the local optical environment
Obtaining time dynamics of the material can be very useful for studying
semiconductor materials used for optoelectronic devices or rare-earth doped
materials
Lifetime Imaging Mod
e
Application of lifetime imaging technique
Lifetime Imaging Mod
e
Cathodoluminescence g(2) imaging
• The g(2) function is a useful tool to study cathodoluminescence emission
from a (nano)material
• In a beam of light, the distribution of photons can be described by the
normalized second order autocorrelation function g (2) (𝜏)
g(2) Imaging Mode
Antibunching in cathodoluminescence
A single-photon emitter can only emit one photon at a time and therefore it is impossible t
o observe coincident photons.
When the g(2) function drops below 1 with g(2)(0)= 0, it is referred to as antibunching.
The antibunching effect can be used to identify and characterize quantum sources
of light.
Figure 4: Characteristic g(2) curves for
different cases. The red balls represent a
schematic photon distribution in time for
particular g(2) curves.
g(2) Imaging Mode
g(2) detector
• The most common approach to measure the g(2)(𝜏) is in a Hanbury Brown and Twiss (HBT)
interferometer consisting of a 50/50 beam splitter with two ultrafast single-photon detectors
(SPDs)
• These SPDs generate a single electrical TTL or NIM pulse for every detected photon, which is then registere
d and timed by time-correlator electronics in a time-correlated single-photon scheme (TCSPC)
• The time-resolved module LAB Cube can coupled to the SPARC CL system with fiber coupler
Figure 5: Schematic overview of the DELMIC L
AB Cube system, that can be used for g(2) acqui
sition.
Bunching g(2) curve courtesy of Dr. Sophie Meur
et
(AMOLF, Amsterdam)
g(2) Imaging Mode
Applications of cathodoluminescence g(2) imaging
• g(2) imaging can be used to identify and characterize single-photon emitter at the nanoscale
• The method can be used in fundamental studies on quantum systems and their interaction with
electron beams
• The bunching effect is useful for studying bulk and mesoscopic materials systems including
optoelectronic devices (such as LEDs and solar cells)
Figure 6: Example of g(2) mapping data on InGaN/GaN
nanorods shown in the SEM image (a). (b) The g(2) data
recorded at three colored squares as indicated by the arro
ws in panel (c) which shows SE intensity recorded togethe
r with
the g(2) data set. Maps of (d) lifetime τe, (e) amplitude g(2) (
0)-1 and (f) the probability of excitation γ are also shown. I
f the
data was too noisy to extract these parameters, the pixel
was left white in the map. The contours of the nanorods ar
e
indicated by the black lines.
Figure courtesy of Dr. Sophie Meuret (AMOLF, Amsterdam
) g(2) Imaging Mode
Cathodoluminescence detector SPARC
The SPARC platform
+ High-performance
cathodoluminescence detection system
+ Modular design allows for addition of
different detectors and detection paths
+ High-precision alignment stage gives
unprecedented photon yield and
reliability
+ Time-resolved mode makes new types
of research possible
Time-resolved SPARC module the LAB Cube
The LAB Cube
+ Lifetime imaging and antibunching
module for SPARC
+ Gives insight into intrinsic material
properties
+ Intuitive and easy to use software
integration with remote control
capabilities
+ Overnight acquisitions for more
accurate measurements
+ The LAB Cube is coupled to the SPARC
with an optical fiber, using the Fiber
Coupler Module
DELMIC B.V.
Address: Kanaalweg 4, 2628 EB,
Delft, The Netherlands
Website: www.delmic.com
Telephone: +31 (0)15 744 01 58
Email: info@delmic.com
Please visit Delmic’s website to learn more about time-
resolved cathodoluminescence

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What is time-resolved cathodoluminescence?

  • 2. What is time-resolved cathodoluminescence? • Time-resolved cathodoluminescence is a technique in which the time dynamics of the cathodoluminescence emission process is observed • Main imaging techniques: 1. Lifetime imaging 2. g(2) imaging
  • 3. How does cathodoluminescence work? When a sample is bombarded by fast electrons, the material becomes excited as it returns to a grounded state, it emits light. The radiation that is generated in the ultraviolet/visible/near-infrared regime of the electromagnetic spectrum is referred to as cathodoluminescence (CL) as the radiation is generated by cathode rays (fast electrons). This data can be collected with nanoscale resolution and can reveal contrasts that cannot be observed with any optical microscopy technique.
  • 4. Lifetime cathodoluminescence imaging • Lifetime (or decay trace) mapping is one of the time-resolved techniques • The method can be used to obtain insight into a large variety of physical processes and material properties • To perform lifetime cathodoluminescence imaging, a pulsed electron microscope is required Lifetime Imaging Mod e
  • 5. Spontaneous light emission process in time Lifetime Imaging Mod e
  • 6. To study lifetime imaging, a fast photodetector such as an avalanche photodiode (APD) or photomultiplier tube (PMT) can be used to detect single photons with high sensitivity and timing- precision Detection Lifetime Imaging Mod e
  • 7. Application of lifetime imaging technique CL decay-trace measurements can be used for a large range of applications The extracted lifetime measurements are valuable to obtain information on intrinsic material properties as well as the local optical environment Obtaining time dynamics of the material can be very useful for studying semiconductor materials used for optoelectronic devices or rare-earth doped materials Lifetime Imaging Mod e
  • 8. Application of lifetime imaging technique Lifetime Imaging Mod e
  • 9. Cathodoluminescence g(2) imaging • The g(2) function is a useful tool to study cathodoluminescence emission from a (nano)material • In a beam of light, the distribution of photons can be described by the normalized second order autocorrelation function g (2) (𝜏) g(2) Imaging Mode
  • 10. Antibunching in cathodoluminescence A single-photon emitter can only emit one photon at a time and therefore it is impossible t o observe coincident photons. When the g(2) function drops below 1 with g(2)(0)= 0, it is referred to as antibunching. The antibunching effect can be used to identify and characterize quantum sources of light. Figure 4: Characteristic g(2) curves for different cases. The red balls represent a schematic photon distribution in time for particular g(2) curves. g(2) Imaging Mode
  • 11. g(2) detector • The most common approach to measure the g(2)(𝜏) is in a Hanbury Brown and Twiss (HBT) interferometer consisting of a 50/50 beam splitter with two ultrafast single-photon detectors (SPDs) • These SPDs generate a single electrical TTL or NIM pulse for every detected photon, which is then registere d and timed by time-correlator electronics in a time-correlated single-photon scheme (TCSPC) • The time-resolved module LAB Cube can coupled to the SPARC CL system with fiber coupler Figure 5: Schematic overview of the DELMIC L AB Cube system, that can be used for g(2) acqui sition. Bunching g(2) curve courtesy of Dr. Sophie Meur et (AMOLF, Amsterdam) g(2) Imaging Mode
  • 12. Applications of cathodoluminescence g(2) imaging • g(2) imaging can be used to identify and characterize single-photon emitter at the nanoscale • The method can be used in fundamental studies on quantum systems and their interaction with electron beams • The bunching effect is useful for studying bulk and mesoscopic materials systems including optoelectronic devices (such as LEDs and solar cells) Figure 6: Example of g(2) mapping data on InGaN/GaN nanorods shown in the SEM image (a). (b) The g(2) data recorded at three colored squares as indicated by the arro ws in panel (c) which shows SE intensity recorded togethe r with the g(2) data set. Maps of (d) lifetime τe, (e) amplitude g(2) ( 0)-1 and (f) the probability of excitation γ are also shown. I f the data was too noisy to extract these parameters, the pixel was left white in the map. The contours of the nanorods ar e indicated by the black lines. Figure courtesy of Dr. Sophie Meuret (AMOLF, Amsterdam ) g(2) Imaging Mode
  • 13. Cathodoluminescence detector SPARC The SPARC platform + High-performance cathodoluminescence detection system + Modular design allows for addition of different detectors and detection paths + High-precision alignment stage gives unprecedented photon yield and reliability + Time-resolved mode makes new types of research possible
  • 14. Time-resolved SPARC module the LAB Cube The LAB Cube + Lifetime imaging and antibunching module for SPARC + Gives insight into intrinsic material properties + Intuitive and easy to use software integration with remote control capabilities + Overnight acquisitions for more accurate measurements + The LAB Cube is coupled to the SPARC with an optical fiber, using the Fiber Coupler Module
  • 15. DELMIC B.V. Address: Kanaalweg 4, 2628 EB, Delft, The Netherlands Website: www.delmic.com Telephone: +31 (0)15 744 01 58 Email: info@delmic.com Please visit Delmic’s website to learn more about time- resolved cathodoluminescence