Enabling Narrow Emission Line Widths in Colloidal Nanocrystals through Coalescence Growth

2020 ◽  
Vol 32 (17) ◽  
pp. 7524-7534
Author(s):  
James Cassidy ◽  
Cole Ellison ◽  
Jacob Bettinger ◽  
Mingrui Yang ◽  
Pavel Moroz ◽  
...  
2020 ◽  
Vol 56 (45) ◽  
pp. 6130-6133 ◽  
Author(s):  
Xiao Jin ◽  
Kanlin Xie ◽  
Tingting Zhang ◽  
Huada Lian ◽  
Zhenghe Zhang ◽  
...  

ZnCdSe/ZnSe quantum dots reveal a notable FWHM of 17.1 nm with a near-unity PL QY at 631 nm.


2007 ◽  
Vol 3 (S245) ◽  
pp. 233-234
Author(s):  
A. Beifiori ◽  
E. M. Corsini ◽  
E. Dalla Bontà ◽  
A. Pizzella ◽  
L. Coccato ◽  
...  

AbstractThe growth of supermassive black holes (SMBHs) appears to be closely linked with the formation of spheroids. There is a pressing need to acquire better statistics on SMBH masses, since the existing samples are preferentially weighted toward early-type galaxies with very massive SMBHs. With this motivation we started a project aimed at measuring upper limits on the mass of the SMBHs that can be present in the center of all the nearby galaxies (D < 100 Mpc) for which STIS/G750M spectra are available in the HST archive. These upper limits will be derived by modeling the central emission-line widths ([N II] λλ6548, 6583, Hα and [S II] λλ6716, 6731) observed over an aperture of ~01 (R < 50 pc). Here we present our preliminary results for a subsample of 76 bulges.


2001 ◽  
Vol 35 (3) ◽  
pp. 360-364 ◽  
Author(s):  
A. N. Imenkov ◽  
N. M. Kolchanova ◽  
P. Kubat ◽  
K. D. Moiseev ◽  
C. Civiš ◽  
...  

2018 ◽  
Vol 482 (2) ◽  
pp. 1889-1899 ◽  
Author(s):  
M-X Wang ◽  
A-L Luo ◽  
Y-H Song ◽  
S-Y Shen ◽  
S Feng ◽  
...  

1989 ◽  
Vol 134 ◽  
pp. 316-317
Author(s):  
S.M. Viegas-Aldrovandi ◽  
M. Contini

In the last decade, emission-lines from a large number of active galactic nuclei (AGN) have been observed. Most of the models built to explain the observed narrow emission-lines are based on photoionization. Although these photoionization models account for the observed general features, many points remain unexplained and several authors suggest an additional energy source (Ferland and Mushotzky 1984, Ferland and Osterbrock 1986, Stasinska 1984, Viegas-Aldrovandi and Gruenwald 1988). Another possible explanation is suggested by the emitting cloud motions, which account for the observed line widths. If the clouds are moving throughout a dilute gas (n0 ≃ 300 cm−3), a shock can develop. Then, the physical conditions in the cloud are determined by the coupled effect of photoionization and shock hydrodynamics.


2007 ◽  
Vol 668 (2) ◽  
pp. 730-737 ◽  
Author(s):  
S. B. Kraemer ◽  
M. C. Bottorff ◽  
D. M. Crenshaw

1986 ◽  
Vol 91 ◽  
pp. 1026 ◽  
Author(s):  
M. M. de Robertis ◽  
R. W. Pogge

1989 ◽  
Vol 343 ◽  
pp. 78 ◽  
Author(s):  
M. Contini ◽  
S. M. Viegas-Aldrovandi

1987 ◽  
Vol 121 ◽  
pp. 119-126
Author(s):  
Martin J. Ward ◽  
N.P. Carleton ◽  
M. Elvis ◽  
G. Fabbiano ◽  
S.P. Willner ◽  
...  

The continua of type 1 Seyferts from 0.3 to 100 microns have been examined. We focus on the modifying effects of dust, both in terms of absorption and re-radiation. After allowance is made for dust and the presence of extranuclear contributions to the IRAS fluxes, there remains a ubiquitous underlying distribution which we believe to be non-thermal. There is evidence that the thermal infrared components corresponding to hot and warm dust may be associated with the broad and narrow emission line regions.


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