Guangda Niu, Liduo Wang, Rui Gao, Beibei Ma, Haopeng Dong, Yong Qiu. Atomic compositions and molar extinction coefficients of PbSe semiconductor nanocrystals were determined by atomic absorption spectrometry, UV−vis−NIR spectrophotometry, and transmission electron microscopy. Quantum dots for Luminescent Solar Concentrators. ��@ q���1�� d2))[ �CA���J�.�P�B``6[��llll3RPP0 a� ��%8��8+����E�3�3��HT�o�u���6�'���ܡh�^���z j;�+=``,j�d���pL�8�q��� �7F���9�2E3i1�p~`{P���,��6{��� �10����{ |� vf���3 0 �� Lei Zhang, Jihong Du, Jun Zhang, Youjin Zheng. ��9���L�(1:jm�5��@��:�@�S�8�*��h�ڠ%�4�HKOE*P�ґ���s�A��J�b����c)��(&K���t-�Ĵ@#�Hp4c��$}����qh���������{I��azX�C�I�3����s�X�b��Ʋ3=���Xđ�>6���[.�c�,��9��`h�8�D���@t����X:$Gm067�Ǐ?��Y�ԁ�-��xw-�e�f�G���d��y�T�$/>��9=*�w�85g���C�P*ڴ8�b�k*�޳��ys=��������I�!�R�]�eu��X+{=����O{��$��0�ќ�o�r��ţYz�M�4ٿ�&��I.�7;�}����P���Rd����%6*���%���^�4�K!iB��Qƀ�ҡ%'5.�����H�`�?�>qh@h}�(6��a���s2T�eT��{2֡��5�Bo?����c. Quanqin Dai, Yingnan Wang, Xinbi Li, Yu Zhang, Donald J. Pellegrino, Muxun Zhao, Bo Zou, JaeTae Seo, Yiding Wang and William W. Yu . without permission from the American Chemical Society. However, the thus obtained “effective absorption coefficient” is advantageous for modeling solely photocurrent‐based devices like solar cells and photodetectors, and to perform detailed balance analysis to determine the open circuit voltage of the solar cells and thermodynamic limit of the detectivity of the photodetectors. Xiaojun Chang and Peter J. Vikesland . Wenqin Shi, Stephan W. H. Eijt, C. S. Suchand Sandeep, Laurens D. A. Siebbeles, Arjan J. Houtepen, Sachin Kinge, Ekkes Brück, Bernardo Barbiellini, Arun Bansil. Xiaojun Chang, W. Matthew Henderson, and Dermont C. Bouchard . You’ve supercharged your research process with ACS and Mendeley! redistribute this material, requesters must process their own requests via the RightsLink permission Quantum Dot Photovoltaics in the Extreme Quantum Confinement Regime: The Surface-Chemical Origins of Exceptional Air- and Light-Stability. K. Nazeeruddin, Michael Grätzel, Sang Il Seok. These are called band gaps. Lisa M. Harris, Eric C. Y. Tam, Struan J. W. Cummins, Martyn P. Coles, and J. Robin Fulton . At λm, the transfer matrix calculates A″′ using κ(λm‐1) as the initial guess of the attenuation coefficient. Buonassisi (MIT) 2011 Light Absorption (and Optical Losses) Lecture3 – 9/15/2011. not otherwise permitted to reproduce, republish, redistribute, or sell any Supporting Information More details on the application itself will be discussed in section 9.6.6. Physica E: Low-dimensional Systems and Nanostructures. Materials Science and Engineering: R: Reports. The multiphoton direct laser writing (DLW) technique offers a means to form 3D structures out of photosensitive materials at the micro and nanoscale, down to resolutions as low as sub-100 nm [45]. Taking into account graphene’s nonlinearity and hydrocarbon contamination, the real transmittance shows that the graphene layer is less transparent at shorter wavelengths (Geim and Novoselov, 2007; Nair et al., 2008). Recently, graphene has emerged as the replacement for SWNTs, providing a comparable nonlinear saturation effect (Wang et al., 2008; Bao et al., 2009; Sun et al., 2010; Zhang et al., 2009). Sorry, we don't have an article for that keyword! the Altmetric Attention Score and how the score is calculated. It showed that the nonlinear absorption could be associated with two-photon absorption at a wavelength of 1064 nm, which the nonlinear refraction was associated with Kerr effect. Somewhat above the band gap energy, the absorption length can drop to the order of a micrometer. 7.3. (If you later retract your consent, we will delete those inputs.) Ali Hreibi, Frédéric Gérôme, Jean-Louis Auguste, Yu Zhang, William W. Yu, Jean-Marc Blondy.

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