The coupling between single 1.3 mum InAs quantum dots (QDs) and photonic crystal nanocavities with quality factors Q up to 15000 is showed. In this condition the Purcell effect (increased spontaneous emission rate) is observed for the first time at these wavelengths. This result is an important step for the development of semiconductor based single photon sources at telecom wavelength, a fundamental need for application like quantum cryptography and quantum computing
The development of semiconductor based single photon sources at telecom wavelength is a fundamental ...
The development of semiconductor based single photon sources at telecom wavelength is a fundamental ...
The authors demonstrate coupling at 1.3 micro m between single InAs quantum dots (QDs) and a mode of...
The coupling between single 1.3 mum InAs quantum dots (QDs) and photonic crystal nanocavities with q...
The coupling between single 1.3 mum InAs quantum dots (QDs) and photonic crystal nanocavities with q...
The coupling between single 1.3 mum InAs quantum dots (QDs) and photonic crystal nanocavities with q...
The coupling between single 1.3 mum InAs quantum dots (QDs) and photonic crystal nanocavities with q...
We show coupling between single 1.3 µm InAs quantum dots (QDs) and photonic crystal nanocavities wit...
We show coupling between single 1.3 µm InAs quantum dots (QDs) and photonic crystal nanocavities wit...
We show coupling between single 1.3 µm InAs quantum dots (QDs) and photonic crystal nanocavities wit...
We show coupling between single 1.3 µm InAs quantum dots (QDs) and photonic crystal nanocavities wit...
The authors demonstrate coupling at 1.3 micro m between single InAs quantum dots (QDs) and a mode of...
The development of semiconductor based single photon sources at telecom wavelength is a fundamental ...
The development of semiconductor based single photon sources at telecom wavelength is a fundamental ...
The development of semiconductor based single photon sources at telecom wavelength is a fundamental ...
The development of semiconductor based single photon sources at telecom wavelength is a fundamental ...
The development of semiconductor based single photon sources at telecom wavelength is a fundamental ...
The authors demonstrate coupling at 1.3 micro m between single InAs quantum dots (QDs) and a mode of...
The coupling between single 1.3 mum InAs quantum dots (QDs) and photonic crystal nanocavities with q...
The coupling between single 1.3 mum InAs quantum dots (QDs) and photonic crystal nanocavities with q...
The coupling between single 1.3 mum InAs quantum dots (QDs) and photonic crystal nanocavities with q...
The coupling between single 1.3 mum InAs quantum dots (QDs) and photonic crystal nanocavities with q...
We show coupling between single 1.3 µm InAs quantum dots (QDs) and photonic crystal nanocavities wit...
We show coupling between single 1.3 µm InAs quantum dots (QDs) and photonic crystal nanocavities wit...
We show coupling between single 1.3 µm InAs quantum dots (QDs) and photonic crystal nanocavities wit...
We show coupling between single 1.3 µm InAs quantum dots (QDs) and photonic crystal nanocavities wit...
The authors demonstrate coupling at 1.3 micro m between single InAs quantum dots (QDs) and a mode of...
The development of semiconductor based single photon sources at telecom wavelength is a fundamental ...
The development of semiconductor based single photon sources at telecom wavelength is a fundamental ...
The development of semiconductor based single photon sources at telecom wavelength is a fundamental ...
The development of semiconductor based single photon sources at telecom wavelength is a fundamental ...
The development of semiconductor based single photon sources at telecom wavelength is a fundamental ...
The authors demonstrate coupling at 1.3 micro m between single InAs quantum dots (QDs) and a mode of...