Influence of Quantum Confinement on the Photoemission From Nonlinear Optical Materials

1997 ◽  
Vol 484 ◽  
Author(s):  
Amakhya P. Ghatak ◽  
P. K. Bose ◽  
Gautam Majumder
Keyword(s):  
Quantum Dots ◽  
Film Thickness ◽  
Quantum Confinement ◽  
Optical Materials ◽  
Nonlinear Optical ◽  
Nonlinear Optical Materials ◽  
Dispersion Law ◽  
Quantum Well Wires ◽  
Electron Dispersion ◽  
Theoretical Results

Abstractwells (QWs), quantum well wires (QWWs) and quantum dots (QDs) of nonlinear optical materials, respectively on the basis of a newly derived electron dispersion law considering all types of anisotropies within the framework of k.p. formalism. It is found, taking CdGeAs2, GaAs and InAs, as exmaples, that the photoemission increase with increasing photon energy in a ladder like manner and also exhibits oscillatory dependences with changing electron concentration with film thickness respectively for all types of quantum confinement. The photoemission current density is greatest in QDs and least in QWWs. In addition, the theoretical results are in agreement with the experimental observation as reported elsewhere.

On The Photoemission From Quantum Confined Compound Semiconductors

1991 ◽  
Vol 228 ◽  
Author(s):  
Kamakhya P. Ghatak ◽  
B. De
Keyword(s):  
Quantum Dots ◽  
Film Thickness ◽  
Quantum Wells ◽  
Electron Concentration ◽  
Quantum Confinement ◽  
Compound Semiconductors ◽  
Dispersion Law ◽  
Quantum Well Wires ◽  
Electron Dispersion ◽  
Theoretical Results

ABSTRACTIn this paper, we have studied the photoemission from quantum wells (QWs), quantum well wires (QWWs) and quantum dots (QDs) of degenerate Kane-type semiconductors, on the basis of a newly derived electron dispersion law considering all types of anisotropies within the framework of k.p formalism. It is found, taking n-Cd3 As2 as an example, that the photoemission increases with increasing photon energy in a ladder-like manner and also exhibits oscillatory dependences with changing electron concentration and with film thickness, for all types of quantum confinement. The photoemission current density is greatest in QDs and least in QWWs. In addition, the theoretical results are in agreement with the experimental observation as reported elsewhere.

On thon the Photoemission from Quantum Confined Strained III–V Systems

1995 ◽  
Vol 379 ◽  
Author(s):  
Kamakhya P. Ghatak ◽  
B. Nag ◽  
G. Mazumder
Keyword(s):  
Quantum Dots ◽  
Film Thickness ◽  
Quantum Wells ◽  
Electron Concentration ◽  
Quantum Confinement ◽  
Dispersion Law ◽  
Quantum Confined ◽  
Electron Dispersion ◽  
Lattice Matched ◽  
Theoretical Results

ABSTRACTIn this paper we have studied the photoemission from quantum wells (QW), quantum wells wires (QWWs) and quantum dots (QDs) of quantum confined strained III–V compounds on the basis of a newly formulated electron dispersion law. It is found taking such quantum confined Hg1–xCdxTe and In1–xGaxAsyP1–y lattice matched InP as examples that the photoemission increases with increasing energy of the incident photons in a ladder like manner and also exhibits oscillatory dependences with changing electron concentration and film thickness respectively for all types quantum confinement. The photoemitted current is greatest in strained QDs and least in unstrained QWs. In addition the theoretical results are in agreement with the experimental datas as given elsewhere.

Thermoelectric Power in Quantum Confined Bismuth Under Classically Large Magnetic Field

1990 ◽  
Vol 216 ◽  
Author(s):  
Kamakhya P. Ghatak ◽  
S. N. Biswas
Keyword(s):  
Magnetic Field ◽  
Quantum Dots ◽  
Quantum Well ◽  
Film Thickness ◽  
Quantum Wells ◽  
Thermoelectric Power ◽  
Large Magnetic Field ◽  
Quantum Well Wires ◽  
Electron Dispersion ◽  
Theoretical Results

ABSTRACTIn this paper we studied the thermoelectric power under classically large magnetic field (TPM) in quantum wells (QWs), quantum well wires (QWWS) and quantum dots (QDs) of Bi by formulating the respective electron dispersion laws. The TPM increases with increasing film thickness in an oscillatory manner in all the cases. The TPM in QD is greatest and the least for quantum wells respectively. The theoretical results are in agreement with the experimental observations as reported elsewhere.

Thermoelectric Power in Quantum Confined Optoelectronic Materials under Classically Large Magnetic Field

1990 ◽  
Vol 181 ◽  
Author(s):  
Kamakhya P. Ghatak ◽  
B. De ◽  
M. Mondal ◽  
S. N. Biswas
Keyword(s):  
Magnetic Field ◽  
Quantum Dots ◽  
Quantum Wells ◽  
Thermoelectric Power ◽  
Optoelectronic Materials ◽  
Large Magnetic Field ◽  
Dispersion Law ◽  
Quantum Well Wires ◽  
Electron Dispersion ◽  
Theoretical Results

ABSTRACTWe shall study the thermoelectric power under classically large magnetic field (TPM) in optoelectronic materials of quantum wells (QWs), quantum well wires (QWW’s), quantum dots (QDs) and compare the same with the hulk specimens of optoelectronic materials by formulating the respective electron dispersion law. The TPM increases with decreasing electron concentration in an oscillatory manner in all the cases, taking n-Hg1-xC dxTe as an example. The TPM in QD is greatest and the least for quantum wells respectively. The theoretical results are in agreement with the experimental observations as reported elsewhere.

Thermoelectric Power in Quantum Confined Optoelectronic Materials under Classically Large Magnetic Field

1990 ◽  
Vol 184 ◽  
Author(s):  
Kamakhya P. Ghatak ◽  
B. De ◽  
M. Mondal ◽  
S. N. Biswas
Keyword(s):  
Magnetic Field ◽  
Quantum Dots ◽  
Quantum Wells ◽  
Thermoelectric Power ◽  
Electron Concentration ◽  
Optoelectronic Materials ◽  
Large Magnetic Field ◽  
Dispersion Law ◽  
Quantum Well Wires ◽  
Electron Dispersion

ABSTRACTWe shall study the thermoelectric power under classically large magnetic field (TPM) in optoelectronic materials of quantum wells (QWs), quantum well wires (QWW's), quantum dots (QDs) and compare the same with the bulk specimens of optoelectronic materials by formulating the respective electron dispersion law. The TPM increases with decreasing electron concentration in an oscillatory manner in all the cases, taking n-Hg1−xCdxTe as an example. The TPM in QD is greatest and the least for quantum wells respectively. The thecoretical results are in agreement with the experimental observations as reported elsewhere.

On the Moss-Burstein Shift In Quantum Confined Optoelectronic Ternary and Quaternary Materials

1997 ◽  
Vol 484 ◽  
Author(s):  
Vamakhya P. Ghatak ◽  
P. K. Bose ◽  
Gautam Majumder
Keyword(s):  
Quantum Dots ◽  
Film Thickness ◽  
Quantum Wires ◽  
Dispersion Law ◽  
Heavy Doping ◽  
Quantum Confined ◽  
Electron Dispersion ◽  
Lattice Matched

AbstractIn this paper we have studied the Burstein-Moss shift in quantum wires and dots of ternary and quaternary materials on the basis of a newly formulated electron dispersion law which occurs as a consequence of heavy doping. It is found taking Hg1−xCdxTe and In1−xGaxAsyP1−y lattice matched to InP as examples that the Burstein-Moss shift exhibits oscillatory dependences for quantum wires and dots of the said materials with respect to doping and film thickness respectively. Besides, the numerical values of the same shift is greatest in quantum dots and least in quantum wires. In addition, the theroretical analysis is in agreement with the experimental datas as given elsewhere.

Heat capacity in quantum dots of nonlinear optical materials

1990 ◽  
Author(s):  
Kamakhya P. Ghatak ◽  
Ardhendhu Ghoshal ◽  
Sankar Bhattacharyya ◽  
Manabendra Mondal
Keyword(s):  
Quantum Dots ◽  
Heat Capacity ◽  
Optical Materials ◽  
Nonlinear Optical ◽  
Nonlinear Optical Materials

First Example of Nonlinear Optical Materials Based on Nanoconjugates of Sandwich Phthalocyanines with Quantum Dots

2017 ◽  
Vol 23 (12) ◽  
pp. 2820-2830 ◽  
Author(s):  
David O. Oluwole ◽  
Alexey V. Yagodin ◽  
Nhlakanipho C. Mkhize ◽  
Kutloano E. Sekhosana ◽  
Alexander G. Martynov ◽  
...  
Keyword(s):  
Quantum Dots ◽  
Optical Materials ◽  
Nonlinear Optical ◽  
Nonlinear Optical Materials
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